Optical image capturing system

ABSTRACT

An optical image capturing system is provided. In the order from an object side to an image side, the optical image capturing system includes a first lens with positive refractive power; a second lens with refractive power; a third lens with refractive power; and a fourth lens with refractive power; and at least one of the image-side surface and object-side surface of each of the four lens elements is aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of Taiwan Patent Application No. 105123107, filed on Jul. 21, 2016, in the Taiwan Intellectual Property Office, the disclosure of which is incorporated herein in its entirety by reference.

BACKGROUND OF THE INVENTION 1. Field of the Invention

The present disclosure relates to an optical image capturing system, and more particularly to a compact optical image capturing system which can be applied to electronic products.

2. Description of the Related Art

In recent years, with the rise of portable electronic devices having camera functionalities, the demand for an optical image capturing system is raised gradually. The image sensing device of ordinary photographing camera is commonly selected from charge coupled device (CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor). In addition, as advanced semiconductor manufacturing technology enables the minimization of pixel size of the image sensing device, the development of the optical image capturing system directs towards the field of high pixels. Therefore, the requirement for high imaging quality is rapidly raised.

The traditional optical image capturing system of a portable electronic device comes with different designs, including a second-lens or a third-lens design. However, the requirement for the higher pixels and the requirement for a large aperture of an end user, like functionalities of micro filming and night view, or the requirement of wide angle of view of the portable electronic device have been raised. But the optical image capturing system with the large aperture design often produces more aberration resulting in the deterioration of quality in peripheral image formation and difficulties of manufacturing, and the optical image capturing system with wide angle of view design increases distortion rate in image formation, thus the optical image capturing system in prior arts cannot meet the requirement of the higher order camera lens module.

Therefore, how to design an optical image capturing system capable of balancing the requirement for higher total pixel count and quality of the formed image as well as the minimization of camera module by effectively increasing the amount of admitted light and the angle of view the optical image capturing system has become a pressing issue.

SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which use combination of refractive powers, convex and concave surfaces of four-piece optical lenses (the convex or concave surface in the disclosure denotes the geometrical shape of an image-side surface or an object-side surface of each lens on an optical axis) and an embedded mechanism element for positioning the lens element to increase the quantity of incoming light of the optical image capturing system and the angle of view of the optical lenses, and to improve total pixels and imaging quality for image formation, so as to be applied to minimized electronic products.

The terminologies together with their numerals for the lens elements parameters related to the embodiment of the present invention are given in the following paragraphs for reference in subsequent illustrations:

The lens element parameter related to the length or height of the lens element A height for image formation of the optical image capturing system is denoted by HOI. A height of the optical image capturing system is denoted by HOS. A distance from the object-side surface of the first lens element to the image-side surface of the fourth lens element is denoted by InTL. A distance from the image-side surface of the fourth lens element to an image plane is denoted by InB, where InTL+InB=HOS. A distance from an aperture stop (aperture) to an image plane is denoted by InS. A distance from the first lens element to the second lens element is denoted by In12 (example). A central thickness of the first lens element of the optical image capturing system on the optical axis is denoted by TP1 (example).

The lens element parameter related to the material in the lens element

An Abbe number of the first lens element in the optical image capturing system is denoted by NA1 (example). A refractive index of the first lens element is denoted by Nd1 (example).

The lens element parameter related to the angle of view of the lens element

The angle of view is denoted by AF. Half of the angle of view is denoted by HAF. A major light angle is denoted by MRA.

The lens element parameter related to exit/entrance pupil in the lens element

An entrance pupil diameter of the optical image capturing system is denoted by HEP. A maximum effective half diameter position of any surface of single lens element means the vertical height between the effective half diameter (EHD) and the optical axis where the incident light of the maximum angle of view of the system passes through the farthest edge of the entrance pupil on the EHD of the surface of the lens element. For example, the maximum effective half diameter position of the object-side surface of the first lens element is denoted as EHD11. The maximum effective half diameter position of the image-side of the first lens element is denoted as EHD12. The maximum effective half diameter position of the object-side surface of the second lens element is denoted as EHD21. The maximum half effective half diameter position of the image-side surface of the second lens element is denoted as EHD22. The maximum effective half diameter position of any surfaces of the remaining lens elements of the optical image capturing system can be referred as mentioned above.

The lens element parameter related to a depth of the lens element shape A distance in parallel with an optical axis from a maximum effective diameter position to an axial point on the object-side surface of the fourth lens element is denoted by InRS41 (example). A distance in parallel with an optical axis from a maximum effective diameter position to an axial point on the image-side surface of the fourth lens element is denoted by InRS42 (example).

The lens element parameter related to the lens element shape

A critical point C is a tangent point on a surface of a specific lens element, and the tangent point is tangent to a plane perpendicular to the optical axis and the tangent point cannot be a crossover point on the optical axis. To follow the past, a distance perpendicular to the optical axis between a critical point C31 on the object-side surface of the third lens element and the optical axis is HVT31 (example). A distance perpendicular to the optical axis between a critical point C32 on the image-side surface of the third lens element and the optical axis is HVT32 (example). A distance perpendicular to the optical axis between a critical point C41 on the object-side surface of the fourth lens element and the optical axis is HVT41 (example). A distance perpendicular to the optical axis between a critical point C42 on the image-side surface of the fourth lens element and the optical axis is HVT42 (example). Distances perpendicular to the optical axis between critical points on the object-side surfaces or the image-side surfaces of other lens elements and the optical axis are denoted in the similar way described above.

The object-side surface of the fourth lens element has one inflection point IF411 which is nearest to the optical axis, and the sinkage value of the inflection point IF411 is denoted by SGI411 (example). SGI411 is a horizontal shift distance in parallel with the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF411 and the optical axis is HIF411 (example). The image-side surface of the fourth lens element has one inflection point IF421 which is nearest to the optical axis and the sinkage value of the inflection point IF421 is denoted by SGI421 (example). SGI421 is a horizontal shift distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF421 and the optical axis is HIF421 (example).

The object-side surface of the fourth lens element has one inflection point IF412 which is the second nearest to the optical axis and the sinkage value of the inflection point IF412 is denoted by SGI412 (example). SGI412 is a horizontal shift distance in parallel with the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the second nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF412 and the optical axis is HIF412 (example). The image-side surface of the fourth lens element has one inflection point IF422 which is the second nearest to the optical axis and the sinkage value of the inflection point IF422 is denoted by SGI422 (example). SGI422 is a horizontal shift distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is the second nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF422 and the optical axis is HIF422 (example).

The object-side surface of the fourth lens element has one inflection point IF413 which is the third nearest to the optical axis and the sinkage value of the inflection point IF413 is denoted by SGI413 (example). SGI413 is a horizontal shift distance in parallel with the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the third nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF413 and the optical axis is HIF413 (example). The image-side surface of the fourth lens element has one inflection point IF423 which is the third nearest to the optical axis and the sinkage value of the inflection point IF423 is denoted by SGI423 (example). SGI423 is a horizontal shift distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is the third nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF423 and the optical axis is HIF423 (example).

The object-side surface of the fourth lens element has one inflection point IF414 which is the fourth nearest to the optical axis and the sinkage value of the inflection point IF414 is denoted by SGI414 (example). SGI414 is a horizontal shift distance in parallel with the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the fourth nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF414 and the optical axis is HIF414 (example). The image-side surface of the fourth lens element has one inflection point IF424 which is the fourth nearest to the optical axis and the sinkage value of the inflection point IF424 is denoted by SGI424 (example). SGI424 is a horizontal shift distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is the fourth nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF424 and the optical axis is HIF424 (example).

The inflection points on the object-side surfaces or the image-side surfaces of the other lens elements and the distances perpendicular to the optical axis thereof or the sinkage values thereof are denoted in the similar way described above.

The lens element parameter related to an aberration

Optical distortion for image formation in the optical image capturing system is denoted by ODT. TV distortion for image formation in the optical image capturing system is denoted by TDT. Further, the range of the aberration offset for the view of image formation may be limited to 50%-100%. An offset of the spherical aberration is denoted by DFS. An offset of the coma aberration is denoted by DFC.

A characteristic diagram of modulation transfer function (MTF) in the optical image capturing system is used to test and evaluate a contrast ratio and a sharpness of image capturing in the system. The vertical coordinate axis of the characteristic diagram of modulation transfer function represents a contrast transfer rate (values are from 0 to 1). The horizontal coordinate axis represents a spatial frequency (cycles/mm; 1 p/mm; line pairs per mm). Theoretically, an ideal image capturing system can show the line contrast of a photographed object by 100%. However, the values of the contrast transfer rate at the vertical coordinate axis are smaller than 1 in the actual image capturing system. The transfer rate of its comparison value is less than a vertical axis. In addition, comparing to the central region, it is generally more difficult to achieve a fine degree of recovery in the edge region of image capturing. The contrast transfer rates (MTF values) with a spatial frequency of 55 cycles/mm of a visible light spectrum at the optical axis, 0.3 field of view and 0.7 field of view on the image plane are respectively denoted by MTFE0, MTFE3 and MTFE7. The contrast transfer rates (MTF values) with a quarter spatial frequency at the optical axis, 0.3 field of view and 0.7 field of view on the image plane are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The contrast transfer rates (MTF values) with half spatial frequency (half frequency) at the optical axis, 0.3 field of view and 0.7 field of view on the image plane are respectively denoted by MTFH0, MTFH3 and MTFH7. The contrast transfer rates (MTF values) with full frequency at the optical axis, 0.3 field of view and 0.7 field of view on the image plane are respectively denoted by MTF0, MTF3 and MTF7. The three fields of view described above are representative to the center, the internal field of view and the external field of view of the lens elements. Thus, they may be used to evaluate whether the performance of a specific optical image capturing system is excellent. The design of the optical image capturing system of the present invention mainly corresponds to a pixel size in which a sensing device below 1.12 micrometers is includes. Therefore, the quarter spatial frequency, the half spatial frequency (half frequency) and the full spatial frequency (full frequency) of the characteristic diagram of modulation transfer function respectively are at least 110 cycles/mm, 220 cycles/mm and 440 cycles/mm.

If an optical image capturing system needs to satisfy with the images aimed to infrared spectrum, such as the requirement for night vision with lower light source, the used wavelength may be 850 nm or 800 nm. As the main function is to recognize shape of an object formed in monochrome and shade, the high resolution is unnecessary, and thus, a spatial frequency, which is less than 100 cycles/mm, is used to evaluate the functionality of the optical image capturing system, when the optical image capturing system is applied to the infrared spectrum. When the foregoing wavelength 850 nm is applied to focus on the image plane, the contrast transfer rates (MTF values) with a spatial frequency of 55 cycles/mm at the optical axis, 0.3 field of view and 0.7 field of view on the image plane are respectively denoted by MTFI0, MTFI3 and MTFI7. However, the infrared wavelength of 850 nm or 800 nm may be hugely different to wavelength of the regular visible light wavelength, and thus, it is hard to design an optical image capturing system which has to focus on the visible light and the infrared light (dual-mode) simultaneously while achieve a certain function respectively.

The disclosure provides an optical image capturing system, wherein an object-side surface or an image-side surface of the fourth lens element has inflection points, such that the angle of incidence from each field of view to the fourth lens element can be adjusted effectively and the optical distortion and the TV distortion can be corrected as well. Besides, the surfaces of the fourth lens element may have a better optical path adjusting ability to acquire better imaging quality.

The disclosure provides an optical image capturing system, in the order from an object side to an image side, including a first, second, third, and fourth lens elements. The first lens element had refractive power. Focal lengths of the first through fourth lens elements are f1, f2, f3 and f4 respectively. A focal length of the optical image capturing system is f. An entrance pupil diameter of the optical image capturing system is HEP. A distance from an object-side surface of the first lens element to the image plane is HOS. The distance on the optical axis from the object-side surface of first lens element to the image-side surface of fourth lens element is denoted by InTL. Half of the maximum viewable angle of the optical image capturing system is denoted by HAF. Thicknesses in parallel with the optical axis of the first, second, third and fourth lens element at the height of ½ HEP respectively are ETP1, ETP2, ETP3 and ETP4. A sum of ETP1 to ETP4 described above is SETP. Central thicknesses of the first, second, third and fourth lens element on the optical axis respectively are TP1, TP2, TP3 and TP4. A sum of TP1 to TP4 described above is STP. The following conditions are satisfied: 1.0≦f/HEP≦10; 0 deg<HAF≦150 deg; and 0.5≦SETP/STP<1.

The disclosure provides another optical image capturing system, in the order from an object side to an image side, including a first, second, third, and fourth lens elements. The first lens element has refractive power. The second lens element has refractive power. The third lens element has refractive power. The fourth lens element has refractive power. At least two lens elements among the first through the fourth lens elements has at least one inflection point on at least one surface thereof. At least one among the second lens element through the fourth lens element has positive refractive power. Focal lengths of the first through fourth lens elements are f1, f2, f3 and f4 respectively. A focal length of the optical image capturing system is f. An entrance pupil diameter of the optical image capturing system is HEP. A distance on the optical axis from an object-side surface of the first lens element to the image plane is HOS. A distance on the optical axis from the object-side surface of the first lens element to the image-side surface of the fourth lens element is InTL. Half of a maximum angle of view of the optical image capturing system is HAF. A horizontal distance in parallel with the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the image plane is ETL. A horizontal distance in parallel with the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN. The following conditions are satisfied: 1.0≦f/HEP≦10.0; 0 deg<HAF≦150 deg and 0.2≦EIN/ETL<1.

The disclosure provides another optical image capturing system, in the order from an object side to an image side, including a first, second, third, and fourth lens elements and an image plane. Among the object-side surface and the image-side surface of the fourth lens element has at least one inflection point on at least one surface thereof. Wherein there are four lens elements with refractive power in the optical image capturing system. The first lens element has refractive power. The second lens element has refractive power. The third lens element has refractive power. The fourth lens element has refractive power. Focal lengths of the first through fourth lens elements are f1, f2, f3 and f4, respectively. A focal length of the optical image capturing system is f. An entrance pupil diameter of the optical image capturing system is HEP. A distance from an object-side surface of the first lens element to the image plane is HOS. A distance on the optical axis from the object-side surface of the first lens element to the image-side surface of the fourth lens element is InTL A horizontal distance in parallel with the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the image plane is ETL. Half of a maximum angle of view of the optical image capturing system is HAF. A horizontal distance in parallel with the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN. The following conditions are satisfied: 1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and 0.2≦EIN/ETL<1.

The thickness of a single lens element at height of ½ entrance pupil diameter (HEP) particularly affects the performance in correcting the optical path difference between the rays in each field of view and in correcting aberration for the shared region among the fields of view within the range of ½ entrance pupil diameter (HEP). The capability of aberration correction is enhanced when the thickness is greater, but the difficulty in manufacturing such lens also increases at the same time. Therefore, it is necessary to control the thickness of a single lens element at height of ½ entrance pupil diameter (HEP), in particular to control the proportional relation (ETP/TP) of the thickness (ETP) of the lens element at height of ½ entrance pupil diameter (HEP) to the thickness (TP) of the corresponding lens element on the optical axis. For example, the thickness of the first lens element at height of ½ entrance pupil diameter (HEP) is denoted by ETP1. The thickness of the second lens element at height of ½ entrance pupil diameter (HEP) is denoted by ETP2. The thicknesses of other lens elements are denoted in similar way. A sum of ETP1 to ETP4 described above is SETP. The embodiments of the present invention may satisfy the following condition: 0.3≦SETP/EIN≦1.

In order to enhance the capability of aberration correction and reduce the difficulty in manufacturing at the same time, it is particularly necessary to control the proportional relationship (ETP/TP) of the thickness (ETP) of the lens element at height of ½ entrance pupil diameter (HEP) to the thickness (TP) of the lens element on the optical axis. For example, the thickness of the first lens element at height of ½ entrance pupil diameter (HEP) is denoted by ETP1. The thickness of the first lens element on the optical axis is TP1. The ratio between both of them is ETP1/TP1. The thickness of the second lens element at height of ½ entrance pupil diameter (HEP) is denoted by ETP2. The thickness of the second lens element on the optical axis is TP2. The ratio between both of them is ETP2/TP2. The proportional relationships of the thicknesses of other lens element in the optical image capturing system at height of ½ entrance pupil diameter (HEP) to the thicknesses (TP) of the lens elements on the optical axis lens are denoted in the similar way. The embodiments of the present invention may satisfy the following condition: 0<ETP/TP≦5.

A horizontal distance between two adjacent lens elements at height of ½ entrance pupil diameter (HEP) is denoted by ED. The horizontal distance (ED) described above is in parallel with the optical axis of the optical image capturing system and particularly affects the corrected aberration of common area of each field of view of light and the capability of optical path difference between each field of view of light at the position of ½ entrance pupil diameter (HEP). The capability of aberration correction may be enhanced if the horizontal distance becomes greater, but the difficulty for manufacturing is also increased and the degree of ‘miniaturization’ to the length of the optical image capturing system is restricted. Thus, it is essential to control the horizontal distance (ED) between two specific adjacent lens elements at height of ½ entrance pupil diameter (HEP).

In order to enhance the capability of aberration correction and reduce the difficulty for ‘miniaturization’ to the length of the optical image capturing system at the same time, it is particularly necessary to control the ratio relation (ED/IN) of the horizontal distance (ED) between the two adjacent lens elements at height of ½ entrance pupil diameter (HEP) to the horizontal distance (IN) between the two adjacent lens elements on the optical axis. For example, the horizontal distance between the first lens element and the second lens element at height of ½ entrance pupil diameter (HEP) is denoted by ED12. The horizontal distance between the first lens element and the second lens element on the optical axis is IN12. The ratio between both of them is ED12/IN12. The horizontal distance between the second lens element and the third lens element at height of ½ entrance pupil diameter (HEP) is denoted by ED23. The horizontal distance between the second lens element and the third lens element on the optical axis is IN23. The ratio between both of them is ED23/IN23. The ratio relations of the horizontal distances between other two adjacent lens elements in the optical image capturing system at height of ½ entrance pupil diameter (HEP) to the horizontal distances between the two adjacent lens elements on the optical axis are denoted in the similar way.

A horizontal distance paralleling the optical axis from a coordinate point on the image-side surface of the fourth lens element at height ½ HEP to the image plane is EBL. A horizontal distance paralleling the optical axis from an axial point on the image-side surface of the fourth lens element to the image plane is BL. The embodiments of the present invention are able to enhance the capability of aberration correction and reserve space to accommodate other optical elements. The following condition may be satisfied: 0.1≦EBL/BL≦1.5.

The optical image capturing system may further include a light filtering element. The light filtering element is located between the fourth lens element and the image plane. A distance paralleling the optical axis from a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP to the light filtering element is EIR. A distance paralleling the optical axis from an axial point on the image-side surface of the fourth lens element to the light filtering element is PIR. The embodiments of the present invention may satisfy the following condition: 0.1≦EIR/PIR≦1.1.

The optical image capturing system described above may be configured to form the image on the image sensing device which is shorter than 1/1.2 inch in diagonal length. The preferred size of the image sensing device is 1/2.3 inch. The pixel size of the image sensing device is smaller than 1.4 micrometers (μm). Preferably the pixel size thereof is smaller than 1.12 micrometers (μm). The best pixel size thereof is smaller than 0.9 micrometers (μm). Furthermore, the optical image capturing system is applicable to the image sensing device with aspect ratio of 16:9.

The optical image capturing system described above is applicable to the demand of video recording with above millions or ten millions-pixels (e.g. 4K and 2K videos or the so-called UHD and QHD) and leads to a good imaging quality.

The height of optical system (HOS) may be reduced to achieve the minimization of the optical image capturing system when the absolute value of f1 is larger than f4 (|f1|>f4).

When the relationship |f2|+|f3|>|f1|+|f4| is satisfied, at least one of the second through third lens elements may have weak positive refractive power or weak negative refractive power. The weak refractive power indicates that an absolute value of the focal length of a specific lens element is greater than 10. When at least one of the second through third lens elements has the weak positive refractive power, the positive refractive power of the first lens element can be shared, such that the unnecessary aberration will not appear too early. On the contrary, when at least one of the second and third lens elements has the weak negative refractive power, the aberration of the optical image capturing system can be corrected and fine-tuned.

The fourth lens element may have negative refractive power, and the image-side surface thereof may be a concave surface. With this configuration, the back focal distance of the optical image capturing system may be shortened and the system may be minimized. Besides, at least one surface of the fourth lens element may possess at least one inflection point, which is capable of effectively reducing the incident angle of the off-axis rays of the field of view, thereby further correcting the off-axis aberration.

BRIEF DESCRIPTION OF THE DRAWINGS

The detailed structure, operating principle and effects of the present disclosure will now be described in more details hereinafter with reference to the accompanying drawings that show various embodiments of the present disclosure as follows.

FIG. 1A is a schematic view of the optical image capturing system according to the first embodiment of the present application.

FIG. 1B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the first embodiment of the present application.

FIG. 1C is a characteristic diagram of modulation transfer of a visible light spectrum according to the first embodiment of the present application.

FIG. 2A is a schematic view of the optical image capturing system according to the second embodiment of the present application.

FIG. 2B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the second embodiment of the present application.

FIG. 2C is a characteristic diagram of modulation transfer of a visible light spectrum according to the second embodiment of the present application.

FIG. 3A is a schematic view of the optical image capturing system according to the third embodiment of the present application.

FIG. 3B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the third embodiment of the present application.

FIG. 3C is a characteristic diagram of modulation transfer of a visible light spectrum according to the third embodiment of the present application.

FIG. 4A is a schematic view of the optical image capturing system according to the fourth embodiment of the present application.

FIG. 4B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the fourth embodiment of the present application.

FIG. 4C is a characteristic diagram of modulation transfer of a visible light spectrum according to the fourth embodiment of the present application.

FIG. 5A is a schematic view of the optical image capturing system according to the fifth embodiment of the present application.

FIG. 5B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the fifth embodiment of the present application.

FIG. 5C is a characteristic diagram of modulation transfer of a visible light spectrum according to the fifth embodiment of the present application.

FIG. 6A is a schematic view of the optical image capturing system according to the sixth embodiment of the present application.

FIG. 6B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the sixth embodiment of the present application.

FIG. 6C is a characteristic diagram of modulation transfer of a visible light spectrum according to the sixth embodiment of the present application.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the exemplary embodiments of the present disclosure, examples of which are illustrated in the accompanying drawings. Therefore, it is to be understood that the foregoing is illustrative of exemplary embodiments and is not to be construed as limited to the specific embodiments disclosed, and that modifications to the disclosed exemplary embodiments, as well as other exemplary embodiments, are intended to be included within the scope of the appended claims. These embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the inventive concept to those skilled in the art. The relative proportions and ratios of elements in the drawings may be exaggerated or diminished in size for the sake of clarity and convenience in the drawings, and such arbitrary proportions are only illustrative and not limiting in any way. The same reference numbers are used in the drawings and the description to refer to the same or like parts.

It will be understood that, although the terms ‘first’, ‘second’, ‘third’, etc., may be used herein to describe various elements, these elements should not be limited by these terms. The terms are used only for the purpose of distinguishing one component from another component. Thus, a first element discussed below could be termed a second element without departing from the teachings of embodiments. As used herein, the term “or” includes any and all combinations of one or more of the associated listed items.

An optical image capturing system, in order from an object side to an image side, includes a first, second, third and fourth lens elements with refractive power. The optical image capturing system may further include an image sensing device which is disposed on an image plane.

The optical image capturing system may use three sets of wavelengths which are 486.1 nm, 587.5 nm and 656.2 nm, respectively, wherein 587.5 nm is served as the primary reference wavelength and a reference wavelength for retrieving technical features. The optical image capturing system may also use five sets of wavelengths which are 470 nm, 510 nm, 555 nm, 610 nm and 650 nm, respectively, wherein 555 nm is served as the primary reference wavelength and a reference wavelength for retrieving technical features.

A ratio of the focal length f of the optical image capturing system to a focal length fp of each of lens elements with positive refractive power is PPR. A ratio of the focal length f of the optical image capturing system to a focal length fn of each of lens elements with negative refractive power is NPR. A sum of the PPR of all lens elements with positive refractive power is ΣPPR. A sum of the NPR of all lens elements with negative refractive powers is ΣNPR. It is beneficial to control the total refractive power and the total length of the optical image capturing system when following conditions are satisfied: 0.5≦ΣPPR/|ΣNPR|≦4.5. Preferably, the following condition may be satisfied: 1≦ΣPPR/|ΣNPR|≦3.5.

The height of the optical image capturing system is HOS. It will facilitate the manufacturing of miniaturized optical image capturing system which may form images with ultra high pixels when the specific ratio value of HOS/f tends to 1.

A sum of a focal length fp of each lens element with positive refractive power is ΣPP. A sum of a focal length fn of each lens element with negative refractive power is ΣNP. In one embodiment of the optical image capturing system of the present disclosure, the following conditions are satisfied: 0<ΣPP≦200 and f1/ΣEPP≦0.85. Preferably, the following conditions may be satisfied: 0<ΣPP≦150 and 0.01≦f1/ΣEPP≦0.7. As a result, the optical image capturing system will have better control over the focusing, and the positive refractive power of the optical system can be distributed appropriately, so as to suppress any premature formation of noticeable aberration.

The first lens element may have positive refractive power, and it has a convex object-side surface. Hereby, the magnitude of the positive refractive power of the first lens element can be fined-tuned, so as to reduce the total track length of the optical image capturing system.

The second lens element may have negative refractive power. Hereby, the aberration generated by the first lens element can be corrected.

The third lens element may have positive refractive power. Hereby, the positive refractive power of the first lens element can be shared.

The fourth lens element may have negative refractive power and a concave image-side surface. With this configuration, the back focal length is reduced in order to keep the size of the optical system small. In addition, at least one of the object-side surface and the image-side surface of the fourth lens element may have at least one inflection point, which is capable of effectively reducing the incident angle of the off-axis rays of the field of view, thereby further correcting the off-axis aberration. Preferably, each of the object-side surface and the image-side surface may have at least one inflection point.

The optical image capturing system may further include an image sensing device which is disposed on an image plane. Half of a diagonal of an effective detection field of the image sensing device (imaging height or the maximum image height of the optical image capturing system) is HOI. A distance on the optical axis from the object-side surface of the first lens element to the image plane is HOS. The following conditions are satisfied: HOS/HOI≦3 and 0.5≦HOS/f≦3.0. Preferably, the following conditions may be satisfied: 1≦HOS/HOI≦2.5 and 1≦HOS/f≦2. Hereby, the miniaturization of the optical image capturing system can be maintained effectively, so as to be carried by lightweight portable electronic devices.

In addition, in the optical image capturing system of the disclosure, according to different requirements, at least one aperture stop may be arranged for reducing stray light and improving the imaging quality.

In the optical image capturing system of the disclosure, the aperture stop may be a front or middle aperture. The front aperture is the aperture stop between a photographed object and the first lens element. The middle aperture is the aperture stop between the first lens element and the image plane. If the aperture stop is the front aperture, a longer distance between the exit pupil and the image plane of the optical image capturing system can be formed, such that more optical elements can be disposed in the optical image capturing system and the efficiency of the image sensing device in receiving images can be improved. If the aperture stop is the middle aperture, the angle of view of the optical image capturing system can be expended, such that the optical image capturing system has the advantage of a wide-angle lens. A distance from the aperture stop to the image plane is InS. The following condition is satisfied: 0.5≦InS/HOS≦1.1. Preferably, the following condition may be satisfied: 0.8≦InS/HOS≦1. Hereby, the size of the optical image capturing system can be kept small without sacrificing the feature of wide angle of view.

In the optical image capturing system of the disclosure, a distance from the object-side surface of the first lens element to the image-side surface of the fourth lens element is InTL. A sum of central thicknesses of all lens elements with refractive power on the optical axis is ΣTP. The following condition is satisfied: 0.45≦ΣTP/InTL≦0.95. Preferably, the following condition may be satisfied: 0.6≦ΣTP/InTL≦0.9. Hereby, contrast ratio for the image formation in the optical image capturing system and defect-free rate for manufacturing the lens element can be given consideration simultaneously, and a proper back focal length is provided to dispose other optical components in the optical image capturing system.

A curvature radius of the object-side surface of the first lens element is R1. A curvature radius of the image-side surface of the first lens element is R2. The following condition is satisfied: 0.01≦|R1/R2|≦0.5. Hereby, the first lens element may have a suitable magnitude of positive refractive power, so as to prevent the longitudinal spherical aberration from increasing too fast. Preferably, the following relation may be satisfied: 0.01≦|R1/R2|≦0.4.

A curvature radius of the object-side surface of the fourth lens element is R9. A curvature radius of the image-side surface of the fourth lens element is R10. The following condition is satisfied: −200<(R7−R8)/(R7+R8)<30. This configuration is beneficial to the correction of the astigmatism generated by the optical image capturing system.

A distance between the first lens element and the second lens element on the optical axis is IN12. The following condition is satisfied: 0<IN12/f≦0.25. Preferably, the following condition may be satisfied: 0.01≦IN12/f≦0.20. Hereby, the chromatic aberration of the lens elements can be mitigated, such that the performance can be increased.

A distance between the second lens element and the third lens element on the optical axis is IN23. The following condition is satisfied: 0≦IN23/f≦0.25. Preferably, the following condition may be satisfied: 0.01≦IN23/f≦0.20. Hereby, the performance of the lens elements can be improved.

A distance between the third lens element and the fourth lens element on the optical axis is IN34. The following condition is satisfied: 0<IN34/f≦0.25. Preferably, the following condition may be satisfied: 0.001≦IN34/f≦0.20. Hereby, the performance of the lens elements can be improved.

Central thicknesses of the first lens element and the second lens element on the optical axis are TP1 and TP2, respectively. The following condition is satisfied: 1≦(TP1+IN12)/TP2≦10. Hereby, the sensitivity produced by the optical image capturing system can be controlled, and the performance can be increased.

Central thicknesses of the third lens element and the fourth lens element on the optical axis are TP3 and TP4, respectively, and a distance between the aforementioned two lens elements on the optical axis is IN34. The following condition is satisfied: 0.2 (TP4+IN34)/TP4≦3. Hereby, the sensitivity produced by the optical image capturing system can be controlled and the total height of the optical image capturing system can be reduced.

A distance between the second lens element and the third lens element on the optical axis is IN23. A total sum of distances from the first lens element to the fourth lens element on the optical axis is ΣTP. The following condition is satisfied: 0.01≦IN23/(TP2+IN23+TP3)≦0.5. Preferably, the following condition may be satisfied: 0.05≦IN23/(TP2+IN23+TP3)≦0.4. Hereby, the aberration generated by the process of moving the incident light can be adjusted slightly layer upon layer, and the total height of the optical image capturing system can be reduced.

In the optical image capturing system of the disclosure, a distance in parallel with an optical axis from a maximum effective diameter position to an axial point on the object-side surface 142 of the fourth lens element is InRS41 (InRS41 is positive if the horizontal displacement is toward the image-side surface, or InRS41 is negative if the horizontal displacement is toward the object-side surface). A distance in parallel with an optical axis from a maximum effective diameter position to an axial point on the image-side surface 144 of the fourth lens element is InRS42. A central thickness of the fourth lens element 140 on the optical axis is TP4. The following conditions are satisfied: −1 mm≦InRS41≦1 mm, −1 mm≦InRS42≦1 mm, 1 mm≦|InRS41|+|InRS42|<2 mm, 0.01≦|InRS41|/TP4≦10 and 0.01≦|InRS42|/TP4≦10. Hereby, the maximum effective diameter position between both surfaces of the fourth lens element can be controlled, so as to facilitate the aberration correction of peripheral field of view of the optical image capturing system and maintain its miniaturization effectively.

In the optical image capturing system of the disclosure, a distance in parallel with an optical axis from an inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI411. A distance in parallel with an optical axis from an inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI421. The following conditions are satisfied: 0<SGI411/(SGI411+TP4)≦0.9 and 0<SGI421/(SGI421+TP4)≦0.9. Preferably, the following conditions may be satisfied: 0.01<SGI411/(SGI411+TP4)≦0.7 and 0.01<SGI421/(SGI421+TP4)≦0.7.

A distance in parallel with the optical axis from the inflection point on the object-side surface of the fourth lens element which is the second nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI412. A distance in parallel with an optical axis from an inflection point on the image-side surface of the fourth lens element which is the second nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI422. The following conditions are satisfied: 0<SGI412/(SGI412+TP4)≦0.9 and 0<SGI422/(SGI422+TP4)≦0.9. Preferably, the following conditions may be satisfied: 0.1≦SGI412/(SGI412+TP4)≦0.8 and 0.1≦SGI422/(SGI422+TP4)≦0.8.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis and the optical axis is denoted by HIF411. A distance perpendicular to the optical axis between an inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis and an axial point on the image-side surface of the fourth lens element is denoted by HIF421. The following conditions are satisfied: 0.01≦HIF411/HOI≦0.9 and 0.01≦HIF421/HOI≦0.9. Preferably, the following conditions may be satisfied: 0.09≦HIF411/HOI≦0.5 and 0.09≦HIF421/HOI≦0.5.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the second nearest to the optical axis and the optical axis is denoted by HIF412. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the second nearest to the optical axis is denoted by HIF422. The following conditions are satisfied: 0.01≦HIF412/HOI≦0.9 and 0.01≦HIF422/HOI≦0.9. Preferably, the following conditions may be satisfied: 0.09≦HIF412/HOI≦0.8 and 0.09≦HIF422/HOI≦0.8.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the third nearest to the optical axis and the optical axis is denoted by HIF413. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the third nearest to the optical axis is denoted by HIF423. The following conditions are satisfied: 0.001 mm≦|HIF413|≦5 mm and 0.001 mm≦|HIF423|≦5 mm. Preferably, the following conditions may be satisfied: 0.1 mm≦|HIF423|≦3.5 mm and 0.1 mm≦|HIF413|≦3.5 mm.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the fourth nearest to the optical axis and the optical axis is denoted by HIF414. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the fourth nearest to the optical axis is denoted by HIF424. The following conditions are satisfied: 0.001 mm≦|HIF414|≦5 mm and 0.001 mm≦|HIF424|≦5 mm. Preferably, the following conditions may be satisfied: 0.1 mm≦|HIF424|≦3.5 mm and 0.1 mm≦|HIF414|≦3.5 mm.

In one embodiment of the optical image capturing system of the present disclosure, the chromatic aberration of the optical image capturing system can be corrected by alternatively arranging the lens elements with large Abbe number and small Abbe number.

The above Aspheric formula is:

z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5) ]+A ₄ h ⁴ +A ₆ h ⁶ +A ₈ h ⁸ +A ₁₀ h ¹⁰ +A ₁₂ h ¹² +A ₁₄ h ¹⁴ +A ₁₆ h ¹⁶ +A ₁₈ h ¹⁸ +A ₂₀ h ²⁰+ . . .  (1),

where z is a position value of the position along the optical axis and at the height h which reference to the surface apex; k is the conic coefficient, c is the reciprocal of curvature radius, and A₄, A₆, A₈, A₁₀, A₁₂, A₁₄, A₁₆, A₁₈, and A₂₀ are high order aspheric coefficients.

The optical image capturing system provided by the disclosure, the lens elements may be made of glass or plastic material. If plastic material is adopted to produce the lens elements, the cost of manufacturing will be lowered effectively. If lens elements are made of glass, the heat effect can be controlled and the designed space arranged for the refractive power of the optical image capturing system can be increased. Besides, the object-side surface and the image-side surface of the first through fourth lens elements may be aspheric, so as to obtain more control variables. Comparing with the usage of traditional lens element made by glass, the number of lens elements used can be reduced and the aberration can be eliminated. Thus, the total height of the optical image capturing system can be reduced effectively.

In addition, in the optical image capturing system provided by the disclosure, if the lens element has a convex surface, the surface of the lens element is convex adjacent to the optical axis. If the lens element has a concave surface, the surface of the lens element is concave adjacent to the optical axis.

Besides, in the optical image capturing system of the disclosure, according to different requirements, at least one aperture may be arranged for reducing stray light and improving the imaging quality.

The optical image capturing system of the disclosure can be adapted to the optical image capturing system with automatic focus if required. With the features of a good aberration correction and a high quality of image formation, the optical image capturing system can be used in various application fields.

The optical image capturing system of the disclosure can include a driving module according to the actual requirements. The driving module may be coupled with the lens elements to enable the lens elements producing displacement. The driving module described above may be the voice coil motor (VCM) which is applied to move the lens to focus, or may be the optical image stabilization (OIS) which is applied to reduce the distortion frequency owing to the vibration of the lens while shooting.

At least one lens element among the first lens element, the second lens element, the third lens element and the fourth lens element of the optical image capturing system of the present disclosure may be a filter element of light with the wavelength of less than 500 nm, according to the actual requirements. The filter element may be made by the coating on at least one surface of the lens element with the specific filtration function or the lens element itself is designed with the material which is able to filter the short wavelength.

The image plane of the present invention may be a plano or a curved surface based on requirement. When the image plane is a curved surface (such as a spherical surface with a curvature radius), it reduces the incident angle the image plane needs to focus light. In addition to achieving reducing the length of the system, it also promotes the relative illumination.

According to the above embodiments, the specific embodiments with figures are presented in detail as below.

The First Embodiment (Embodiment 1)

Please refer to FIG. 1A, FIG. 1B, and FIG. 1C. 1A is a schematic view of the optical image capturing system according to the first embodiment of the present application, FIG. 1B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the first embodiment of the present application, and FIG. 1C is a characteristic diagram of modulation transfer of a visible light spectrum according to the first embodiment of the present application. As shown in FIG. 1A, in the order from an object side to an image side, the optical image capturing system includes a first lens element 110, a second lens element 120, an aperture 100, a third lens element 130, a fourth lens element 140, an IR-bandstop filter 170, an image plane 180, and an image sensing device 190.

The first lens element 110 has positive refractive power and it is made of plastic material. The first lens element 110 has a convex object-side surface 112 and a concave image-side surface 114, and both of the object-side surface 112 and the image-side surface 114 are aspheric and each of them has one inflection point. The central thickness of the first lens element on the optical axis is TP1 while the thickness of the first lens element, paralleling the optical axis, and at height of ½ entrance pupil diameter (HEP) is ETP1.

A distance paralleling an optical axis from an inflection point on the object-side surface of the first lens element which is nearest to the optical axis to an axial point on the object-side surface of the first lens element is denoted by SGI111. A distance paralleling an optical axis from an inflection point on the image-side surface of the first lens element which is nearest to the optical axis to an axial point on the image-side surface of the first lens element is denoted by SGI121. The following conditions are satisfied: SGI111=0.2008 mm, SGI121=0.0113 mm, |SGI111|/(|SGI111|+TP1)=0.3018 and |SGI121|/(|SGI121|+TP1)=0.0238.

A distance perpendicular to the optical axis from the inflection point on the object-side surface of the first lens element which is nearest to the optical axis to an axial point on the object-side surface of the first lens element is denoted by HIF111. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the first lens element which is nearest to the optical axis to an axial point on the image-side surface of the first lens element is denoted by HIF121. The following conditions are satisfied: HIF111=0.7488 mm, HIF121=0.4451 mm, HIF111/HOI=0.2552 and HIF121/HOI=0.1517.

The second lens element 120 has positive refractive power and it is made of plastic material. The second lens element 120 has a concave object-side surface 122 and a convex image-side surface 124, and both of the object-side surface 122 and the image-side surface 124 are aspheric. The object-side surface 122 has an inflection point. The central thickness of the second lens element on the optical axis is TP2 while the thickness paralleling the optical axis of the second lens element at height of ½ entrance pupil diameter (HEP) is ETP2.

A distance paralleling an optical axis from an inflection point on the object-side surface of the second lens element which is nearest to the optical axis to an axial point on the object-side surface of the second lens element is denoted by SGI211. A distance paralleling an optical axis from an inflection point on the image-side surface of the second lens element which is nearest to the optical axis to an axial point on the image-side surface of the second lens element is denoted by SGI221. The following conditions are satisfied: SGI211=−0.1791 mm and |SGI211|/(|SGI211|+TP2)=0.3109.

A distance perpendicular to the optical axis from the inflection point on the object-side surface of the second lens element which is nearest to the optical axis to an axial point on the object-side surface of the second lens element is denoted by HIF211. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the second lens element which is nearest to the optical axis to an axial point on the image-side surface of the second lens element is denoted by HIF221. The following conditions are satisfied: HIF211=0.8147 mm and HIF211/HOI=0.2777.

The third lens element 130 has negative refractive power and it is made of plastic material. The third lens element 130 has a concave object-side surface 132 and a convex image-side surface 134, and both of the object-side surface 132 and the image-side surface 134 are aspheric. The image-side surface 134 has an inflection point. The central thickness of the third lens element on the optical axis is TP3 while the thickness paralleling the optical axis of the third lens element at height of ½ entrance pupil diameter (HEP) is ETP3.

A distance paralleling an optical axis from an inflection point on the object-side surface of the third lens element which is nearest to the optical axis to an axial point on the object-side surface of the third lens element is denoted by SGI311. A distance paralleling an optical axis from an inflection point on the image-side surface of the third lens element which is nearest to the optical axis to an axial point on the image-side surface of the third lens element is denoted by SGI321. The following relationship are satisfied: SGI321=−0.1647 mm; |SGI321|/(|SGI321|+TP3)=0.1884.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens element which is nearest to the optical axis and the optical axis is denoted by HIF311. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the third lens element which is nearest to the optical axis to an axial point on the image-side surface of the third lens element is denoted by HIF321. The following conditions are satisfied: HIF321=0.7269 mm and HIF321/HOI=0.2477.

The fourth lens element 140 has negative refractive power and it is made of plastic material. The fourth lens element 140 has a convex object-side surface 142 and a concave image-side surface 144; both of the object-side surface 142 and the image-side surface 144 are aspheric. The object-side surface 142 thereof has two inflection points while the image-side surface 144 thereof has an inflection point. The central thickness of the fourth lens element on the optical axis is TP4 while the thickness paralleling the optical axis of the fourth lens element at height of ½ entrance pupil diameter (HEP) is ETP4.

A distance paralleling an optical axis from an inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI411. A distance paralleling an optical axis from an inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI421. The following conditions are satisfied: SGI411=0.0137 mm, SGI421=−0.0922 mm, |SGI411|/(|SGI411|+TP4)=0.0155 and |SGI421|/(|SGI421|+TP4)=0.0956.

A distance paralleling an optical axis from an inflection point on the object-side surface of the fourth lens element which is the second nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI412. The following conditions are satisfied: SGI412=−0.1518 mm and |SGI412|/(|SGI412|+TP4)=0.1482.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis and the optical axis is denoted by HIF411. A distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis and the optical axis is denoted by HIF421. The following conditions are satisfied: HIF411=0.2890 mm, HIF421=0.5794 mm, HIF411/HOI=0.0985 and HIF421/HOI=0.1975.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is second nearest to the optical axis and the optical axis is denoted by HIF412. The following conditions are satisfied: HIF412=1.3328 mm and HIF412/HOI=0.4543.

The IR-bandstop filter 170 is made of glass material and is disposed between the fourth lens element 140 and the image plane 180 without affecting the focal length of the optical image capturing system.

In the optical image capturing system of the first embodiment, a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, and half of a maximal view angle of the optical image capturing system is HAF. The detailed parameters are shown as below: f=3.4375 mm, f/HEP=2.23, HAF=39.69° and tan(HAF)=0.8299.

In the optical image capturing system of the first embodiment, a focal length of the first lens element 110 is f1 and a focal length of the fourth lens element 140 is f4. The following conditions are satisfied: f1=3.2736 mm, |f/f1|=1.0501, f4=−8.3381 mm and |f1/f4|=0.3926.

In the optical image capturing system of the first embodiment, a focal length of the second lens element 120 is f2 and a focal length of the third lens element 130 is f3. The following conditions are satisfied: |f2|+|f3|=10.0976 mm, |f1|+|f4|=11.6116 mm and |f2|+|f3|<|f1|+|f4|.

A ratio of the focal length f of the optical image capturing system to a focal length fp of each of the lens elements with positive refractive powers is PPR. A ratio of the focal length f of the optical image capturing system to a focal length fn of each of the lens elements with negative refractive powers is NPR. In the optical image capturing system of the first embodiment, a sum of the PPR of all lens elements with positive refractive powers is ΣPPR=|f/f1|+|f/f2|=1.95585. A sum of the NPR of all lens elements with negative refractive powers is ΣNPR=|f/f3|+|f/f4|=0.95770, ΣPPR/|ΣNPR|=2.04224. The following conditions are also satisfied: |f/f1|=1.05009, |f/f2|=0.90576, |f/f3|=0.54543 and |f/f4|=0.41227.

In the optical image capturing system of the first embodiment, a distance from the object-side surface 112 of the first lens element to the image-side surface 144 of the fourth lens element is InTL. A distance from the object-side surface 112 of the first lens element to the image plane 180 is HOS. A distance from an aperture 100 to an image plane 180 is InS. Half of a diagonal length of an effective detection field of the image sensing device 190 is HOI. A distance from the image-side surface 144 of the fourth lens element to an image plane 180 is InB. The following conditions are satisfied: InTL+InB=HOS, HOS=4.4250 mm, HOI=2.9340 mm, HOS/HOI=1.5082, HOS/f=1.2873; InTL/HOS=0.7191, InS=4.2128 mm and InS/HOS=0.95204.

In the optical image capturing system of the first embodiment, the sum of central thicknesses of all lens elements with refractive powers on the optical axis is ΣTP. The following conditions are satisfied: ΣTP=2.4437 mm and ΣTP/InTL=0.76793. Therefore, both contrast ratio for the image formation in the optical image capturing system and yield rate of the manufacturing process of the lens element can be balanced, and a proper back focal length is provided to dispose other optical components in the optical image capturing system.

In the optical image capturing system of the first embodiment, a curvature radius of the object-side surface 112 of the first lens element is R1. A curvature radius of the image-side surface 114 of the first lens element is R2. The following condition is satisfied: |R1/R2|=0.1853. Hereby, the first lens element has a suitable magnitude of positive refractive power, so as to prevent the spherical aberration from increasing too fast.

In the optical image capturing system of the first embodiment, a curvature radius of the object-side surface 142 of the fourth lens element is R7. A curvature radius of the image-side surface 144 of the fourth lens element is R8. The following condition is satisfied: (R7−R8)/(R7+R8)=0.2756. As such, the astigmatism generated by the optical image capturing system can be corrected.

In the optical image capturing system of the first embodiment, the focal lengths for the first lens element 110 and the second lens element 120 are respectively f1 and f2. The sum of the focal lengths for all lens elements having positive refractive power is ΣPP, which satisfies the following conditions: ΣPP=f1+f2=7.0688 mm and f1/(f1+f2)=0.4631. Therefore, the positive refractive power of the first lens element 110 may be distributed to other lens elements with positive refractive power appropriately, so as to suppress the generation of noticeable aberrations along the path of travel of the incident light in the optical image capturing system.

In the optical image capturing system of the first embodiment, the focal lengths for the third lens element 130 and the fourth lens element 140 are respectively f3 and f4. The sum of the focal lengths for all lens elements having negative refractive powers is ΣNP, which satisfies the following conditions: ΣNP=f3+f4=−14.6405 mm and f4/(f2+f4)=0.5695. Therefore, the negative refractive power of the fourth lens element may be distributed to other lens elements with negative refractive power appropriately, so as to suppress the generation of noticeable aberrations along the path of travel of the incident light in the optical image capturing system.

In the optical image capturing system of the first embodiment, a distance between the first lens element 110 and the second lens element 120 on the optical axis is IN12. The following conditions are satisfied: IN12=0.3817 mm and IN12/f=0.11105. Hereby, the chromatic aberration of the lens elements can be mitigated, such that the performance of the optical system is increased.

In the optical image capturing system of the first embodiment, a distance between the second lens element 120 and the third lens element 130 on the optical axis is IN23. The following conditions are satisfied: IN23=0.0704 mm and IN23/f=0.02048. Hereby, the chromatic aberration of the lens elements can be mitigated, such that the performance of the optical system is increased.

In the optical image capturing system of the first embodiment, a distance between the third lens element 130 and the fourth lens element 140 on the optical axis is IN34. The following conditions are satisfied: IN34=0.2863 mm and IN34/f=0.08330. Hereby, the chromatic aberration of the lens elements can be mitigated, such that the performance of the optical system is increased.

In the optical image capturing system of the first embodiment, central thicknesses of the first lens element 110 and the second lens element 120 on the optical axis are TP1 and TP2, respectively. The following conditions are satisfied: TP1=0.46442 mm, TP2=0.39686 mm, TP1/TP2=1.17023 and (TP1+IN12)/TP2=2.13213. Hereby, the precision of the manufacturing of the optical image capturing system can be controlled, and the performance thereof can be increased.

In the optical image capturing system of the first embodiment, central thicknesses of the third lens element 130 and the fourth lens element 140 on the optical axis are TP3 and TP4, respectively. The separation distance between the third lens element 130 and the fourth lens element 140 on the optical axis is IN34. The following conditions are satisfied: TP3=0.70989 mm, TP4=0.87253 mm, TP3/TP4=0.81359 and (TP4+IN34)/TP3=1.63248. Hereby, the precision of the manufacturing of the optical image capturing system can be controlled, and the total height of the optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, the following relations are satisfied: IN23/(TP2+IN23+TP3)=0.05980. Hereby, the aberration generated along the path of travel of the incident light inside the optical system can be slightly corrected by successive lens elements, and the total height of the optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, a distance paralleling an optical axis from a maximum effective diameter position to an axial point on the object-side surface 142 of the fourth lens element is InRS41. A distance paralleling an optical axis from a maximum effective diameter position to an axial point on the image-side surface 144 of the fourth lens element is InRS42. A central thickness of the fourth lens element 140 is TP4. The following conditions are satisfied: InRS41=−0.23761 mm, InRS42=−0.20206 mm, InRS41+|InRS42|=0.43967 mm, |InRS41|/TP4=0.27232 and |InRS42|/TP4=0.23158. Hereby, it is favorable to the manufacturing and molding of the lens element, while maintaining the minimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, a distance perpendicular to the optical axis between a critical point C41 on the object-side surface 142 of the fourth lens element and the optical axis is HVT41. A distance perpendicular to the optical axis between a critical point C42 on the image-side surface 144 of the fourth lens element and the optical axis is HVT42. The following conditions are satisfied: HVT41=0.5695 mm, HVT42=1.3556 mm and HVT41/HVT42=0.4201. With this configuration, the off-axis aberration could be corrected effectively.

In the optical image capturing system of the first embodiment, the following condition is satisfied: HVT42/HOI=0.4620. As such, the aberration at the surrounding field of view of the optical image capturing system may be corrected effectively.

In the optical image capturing system of the first embodiment, the following condition is satisfied: HVT42/HOS=0.3063. As such, the aberration at the surrounding field of view of the optical image capturing system may be corrected effectively.

In the optical image capturing system of the first embodiment, the Abbe number of the first lens element is NA1. The Abbe number of the second lens element is NA2. The Abbe number of the third lens element is NA3. The Abbe number of the fourth lens element is NA4. The following conditions are satisfied: |NA1−NA2|=0 and NA3/NA2=0.39921. Hereby, the chromatic aberration of the optical image capturing system can be corrected.

In the optical image capturing system of the first embodiment, TV distortion and optical distortion for image formation in the optical image capturing system are TDT and ODT, respectively. The following conditions are satisfied: |TDT|=0.4% and |ODT|=2.5%.

In the optical image capturing system of the present embodiment, the contrast transfer rates of modulation transfer (values of MTF) of half frequency at positions of the optical axis, 0.3 HOI and 0.7 HOI on the image plane are respectively denoted by MTFH0, MTFH3 and MTFH7. The following conditions are satisfied: MTFH0 is about 0.525, MTFH3 is about 0.375, and MTFH7 is about 0.35.

Please refer to the following Table 1 and Table 2.

The detailed data of the optical image capturing system of the first embodiment is as shown in Table 1.

TABLE 1 Lens Parameters for the First Embodiment f = 3.4375 mm, f/HEP = 2.23, HAF = 39.6900 deg; tan(HAF) = 0.8299 Central Refractive Focal Surface # Curvature Radius Thickness Material Index Abbe # length 0 Object Plano ∞ 1 Lens 1/ 1.466388 0.464000 Plastic 1.535 56.07 3.274 Ape. stop 2 7.914480 0.382000 3 Lens 2 −5.940659 0.397000 Plastic 1.535 56.07 3.795 4 −1.551401 0.070000 5 Lens 3 −0.994576 0.710000 Plastic 1.642 22.46 −6.302 6 −1.683933 0.286000 7 Lens 4 2.406736 0.873000 Plastic 1.535 56.07 −8.338 8 1.366640 0.213000 9 IR-bandstop Plano 0.210000 BK7_SCHOTT 1.517 64.13 filter 10 Plano 0.820000 11 Image plane Plano Reference wavelength = 555 nm, shield position: The 8^(th) surface with clear aperture of 2.320 mm. As for the parameters of the aspheric surfaces of the first embodiment, reference is made to Table 2.

TABLE 2 Aspheric Coefficients Surface # 1 2 3 4 5 6 k = −1.595426E+00 −7.056632E+00 −2.820679E+01 −1.885740E+00 1.013988E−01 −3.460337E+01 A₄ = −4.325520E−04 −2.633963E−02 −1.367865E−01 −9.745260E−02 2.504976E−01 −9.580611E−01 A₆ =  1.103749E+00  2.088207E−02  3.135755E−01 −1.032177E+00 −1.640463E+00   3.303418E+00 A₈ = −8.796867E+00 −1.122861E−01 −6.149514E+00  8.016230E+00 1.354700E+01 −8.544412E+00 A₁₀ =  3.981982E+01 −7.137813E−01  3.883332E+01 −4.215882E+01 −6.223343E+01   1.602487E+01 A₁₂ = −1.102573E+02  2.236312E+00 −1.463622E+02  1.282874E+02 1.757259E+02 −2.036011E+01 A₁₄ =  1.900642E+02 −2.756305E+00  3.339863E+02 −2.229568E+02 −2.959459E+02   1.703516E+01 A₁₆ = −2.000279E+02  1.557080E+00 −4.566510E+02  2.185571E+02 2.891641E+02 −8.966359E+00 A₁₈ =  1.179848E+02 −2.060190E+00  3.436469E+02 −1.124538E+02 −1.509364E+02   2.684766E+00 A₂₀ = −3.023405E+01  2.029630E+00 −1.084572E+02  2.357571E+01 3.243879E+01 −3.481557E−01 Surface # 7 8 k = −4.860907E+01 −7.091499E+00 A₄ = −2.043197E−01 −8.148585E−02 A₆ =  6.516636E−02  3.050566E−02 A₈ =  4.863926E−02 −8.218175E−03 A₁₀ = −7.086809E−02  1.186528E−03 A₁₂ =  3.815824E−02 −1.305021E−04 A₁₄ = −1.032930E−02  2.886943E−05 A₁₆ =  1.413303E−03 −6.459004E−06 A₁₈ = −8.701682E−05  6.571792E−07 A₂₀ =  1.566415E−06 −2.325503E−08

Table 1 is the detailed structure data to the first embodiment in FIG. 1A, wherein the unit of the curvature radius, the thickness, the distance, and the focal length is millimeters (mm). Surfaces 0-11 illustrate the surfaces from the object side to the image plane in the optical image capturing system. Table 2 is the aspheric coefficients of the first embodiment, wherein k is the conic coefficient in the aspheric surface formula, and A₁-A₂₀ are the first to the twentieth order aspheric surface coefficients. Besides, the tables in the following embodiments are referenced to the schematic view and the aberration graphs, respectively, and definitions of parameters in the tables are equal to those in the Table 1 and the Table 2, so the repetitious details will not be given here.

The Second Embodiment (Embodiment 2)

Please refer to FIG. 2A, FIG. 2B, and FIG. 2C. FIG. 2A is a schematic view of the optical image capturing system according to the second embodiment of the present application, FIG. 2B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the second embodiment of the present application, and FIG. 2C is a characteristic diagram of modulation transfer of a visible light spectrum according to the second embodiment of the present application. As shown in FIG. 2A, in the order from an object side to an image side, the optical image capturing system includes an aperture stop 200, a first lens element 210, a second lens element 220, a third lens element 230, a fourth lens element 240, an IR-bandstop filter 270, an image plane 280, and an image sensing device 290.

The first lens element 210 has positive refractive power and it is made of plastic material. The first lens element 210 has a convex object-side surface 212 and a convex image-side surface 214, and both of the object-side surface 212 and the image-side surface 214 are aspheric. The object-side surface 212 thereof has one inflection point.

The second lens element 220 has negative refractive power and it is made of plastic material. The second lens element 220 has a concave object-side surface 222 and a convex image-side surface 224, and both of the object-side surface 222 and the image-side surface 224 are aspheric and each of them has one inflection point.

The third lens element 230 has positive refractive power and it is made of plastic material. The third lens element 230 has a concave object-side surface 232 and a convex image-side surface 234, and both of the object-side surface 232 and the image-side surface 234 are aspheric. The object-side surface 232 of the third lens element 230 has two inflection points while the image-side surface 234 thereof has one inflection point.

The fourth lens element 240 has negative refractive power and it is made of plastic material. The fourth lens element 240 has a convex object-side surface 242 and a concave image-side surface 244, both of the object-side surface 242 and the image-side surface 244 are aspheric. The object-side surface 242 has two inflection points and the image-side surface 244 has an inflection point.

The IR-bandstop filter 270 is made of glass material. The IR-bandstop filter 270 is disposed between the fourth lens element 240 and the image plane 280 without affecting the focal length of the optical image capturing system.

Please refer to the following Table 3 and Table 4.

The detailed data of the optical image capturing system of the second embodiment is as shown in Table 3.

TABLE 3 Lens Parameters for the Second Embodiment f = 2.43567 mm, f/HEP = 2.25, HAF = 42.5398 deg, Central Refractive Focal Surface # Curvature Radius Thickness Material Index Abbe # length 0 Object 1E+18 600 1 Ape. stop 1E+18 −0.007 2 Lens 1 2.933004299 0.837 Plastic 1.535 56.27 1.856 3 −1.356498569 −0.206 4 Lens 2 1E+18 0.530 Plastic 1.636 23.89 −2.471 5 −0.571512432 0.383 6 Lens 3 −1.128950531 0.065 Plastic 1.535 56.27 3.538 7 −370.115347 0.510 8 Lens 4 −1.888885375 0.034 Plastic 1.535 56.27 −29.312 9 1.362024 0.479 10 IR-bandstop 1.09966183 0.436 BK7_SCHOTT 1.517 64.13 filter 11 1E+18 0.650 12 1E+18 0.368 13 Image plane 1E+18 0.000 Reference wavelength = 555 nm; shield position: The 4^(th) surface with clear aperture of 0.820 mm. As for the parameters of the aspheric surfaces of the second embodiment, reference is made to Table 4.

TABLE 4 Aspheric Coefficients Surface # 2 3 4 5 6 7 k = −1.167943E+02 −8.096076E−01 −8.485431E−01 −1.287588E+00 −3.557391E+02 −1.035962E+00 A₄ = 4.062215E−01 −2.135766E−01 3.610508E−01 2.411831E−01 1.465274E−01 6.898240E−02 A₆ = −2.050763E+00 7.739099E−02 3.973776E−01 −3.541967E−02 −1.056315E−01 1.018619E−01 A₈ = 3.165246E+00 −9.812521E−02 −4.766410E−01 −1.493358E−01 2.169853E−02 −1.014282E−01 A₁₀ = 1.042195E+01 −4.037456E−01 −1.379617E+00 7.110098E−02 −2.295577E−02 2.179672E−02 A₁₂ = −5.823624E+01 4.125859E−01 3.645913E+00 3.943633E−02 2.524299E−02 1.489563E−02 A₁₄ = 6.661856E+01 1.795293E−01 −2.191978E+00 −2.433511E−02 −1.133140E−02 −5.681425E−03 A₁₆ = 1.657219E+01 −5.302035E−02 9.624827E−02 1.643650E−03 4.423690E−04 2.751027E−05 Surface # 8 9 k = −7.113039E+00 −7.554711E−01 A₄ = 8.297912E−02 −2.145978E−01 A₆ = −2.435076E−01 −2.781062E−03 A₈ = 1.554465E−01 3.506390E−02 A₁₀ = −5.277254E−02 −1.743476E−02 A₁₂ = 1.405967E−02 3.862285E−03 A₁₄ = −2.876320E−03 −3.613872E−04 A₁₆ = 2.704978E−04 4.807794E−06

In the second embodiment, the presentation of the aspheric surface formula is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are identical to those in the first embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 3 and Table 4.

Second embodiment (Primary reference wavelength = 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.674  0.504  0.430  0.504  1.202  0.601  ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.805  1.315  0.844  1.053  0.939  2.112  ETL EBL EIN EIR PIR STP 4.049  1.336  2.713  0.319  0.436  2.208  EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.670  0.778  0.731  0.9191  1.4536  0.956  ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.221  0.184  0.196  0.683  2.818  5.711  InRS41 InRS42 HVT41 HVT42 ODT % TDT % 0.17447 0.32046 1.08696 1.45500 1.62704 0.64849 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 1.31247 0.98576 0.68839 0.08309 0.75107 0.69834 ΣPPR ΣNPR ΣPPR/| ΣNPR | ΣPP ΣNP f1/ΣPP 1.06886 2.00086 0.53420 −31.78285    5.39399 0.92226 f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f 0.34405 0.13306 0.02680 0.01408 0.20922 0.19651 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL 2.63211 4.08574 1.80147 0.99824 0.64422 0.83905 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 3.02950 1.00657 2.18389 1.06467 0.06812 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS 0.3645  0.6695  0.6415  0.3561  MTFQ0 MTFQ3 MTFQ7 MTFH0 MTFH3 MTFH7 0.82   0.45   0.53   0.63   0.1   0.27  

The following contents may be deduced from Table 3 and Table 4.

Values Related to Inflection Point of Second Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.4053 HIF111/HOI 0.1787 SGI111 0.0246 |SGI111|/(|SGI111| + TP1) 0.0285 HIF211 0.6699 HIF211/HOI 0.2954 SGI211 −0.3294 |SGI211|/(|SGI211| + TP2) 0.4622 HIF221 0.9275 HIF221/HOI 0.4089 SGI221 −0.2485 |SGI221|/(|SGI221| + TP2) 0.3933 HIF311 0.0392 HIF311/HOI 0.0173 SGI311 −0.000002 |SGI311|/(|SGI311| + TP3) 0.000004 HIF312 0.8073 HIF312/HOI 0.3560 SGI312 0.0347 |SGI312/(|SGI312| + TP3) 0.0638 HIF321 0.6347 HIF321/HOI 0.2798 SGI321 −0.0911 |SGI321|/(|SGI321| + TP3) 0.1516 HIF411 0.5903 HIF411/HOI 0.2603 SGI411 0.1056 |SGI411|/(|SGI411| + TP4) 0.1807 HIF412 1.2855 HIF412/HOI 0.5668 SGI412 0.1840 |SGI412|/(|SGI412| + TP4) 0.2777 HIF421 0.6695 HIF421/HOI 0.2952 SGI421 0.1664 |SGI421|/(|SGI421| + TP4) 0.2580

The Third Embodiment (Embodiment 3)

Please refer to FIG. 3A, FIG. 3B, and FIG. 3C. FIG. 3A is a schematic view of the optical image capturing system according to the third embodiment of the present application, FIG. 3B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the third embodiment of the present application, and FIG. 3C is a characteristic diagram of modulation transfer of a visible light spectrum according to the third embodiment of the present application. As shown in FIG. 3A, in the order from an object side to an image side, the optical image capturing system includes an aperture stop 300, a first lens element 310, a second lens element 320, a third lens element 330, a fourth lens element 340, an IR-bandstop filter 370, an image plane 380, and an image sensing device 390.

The first lens element 310 has positive refractive power and it is made of plastic material. The first lens element 310 has a convex object-side surface 312 and a convex image-side surface 314, and both of the object-side surface 312 and the image-side surface 314 are aspheric. The object-side surface 312 has a inflection point.

The second lens element 320 has negative refractive power and it is made of plastic material. The second lens element 320 has a concave object-side surface 322 and a convex image-side surface 324, and both of the object-side surface 322 and the image-side surface 324 are aspheric.

The third lens element 330 has positive refractive power and it is made of plastic material. The third lens element 330 has a concave object-side surface 332 and a convex image-side surface 334, and both of the object-side surface 332 and the image-side surface 334 are aspheric. The object-side surface 332 has two inflection points and the image-side surface 334 has one inflection point.

The fourth lens element 340 has negative refractive power and it is made of plastic material. The fourth lens element 340 has a convex object-side surface 342 and a concave image-side surface 344, and both of the object-side surface 342 and the image-side surface 344 are aspheric, and each of them has one inflection point.

The IR-bandstop filter 370 is made of glass material. The IR-bandstop filter 370 is disposed between the fourth lens element 340 and the image plane 380 without affecting the focal length of the optical image capturing system.

Please refer to the following Table 5 and Table 6.

The detailed data of the optical image capturing system of the third embodiment is as shown in Table 5.

TABLE 5 Lens Parameters for the Third Embodiment f = 2.38369 mm, f/HEP = 2.24, HAF = 43.2532 deg Central Refractive Focal Surface# Curvature Radius Thickness Material Index Abbe # length 0 Object 1E+18 600 1 Ape. 1E+18 −0.041 Stop 2 Lens 1 2.748946552 0.774 Plastic 1.545 55.99 1.696 3 −1.258232969 −0.216 4 Lens 2 1E+18 0.442 Plastic 1.643 22.47 −1.830 5 −0.708007484 0.364 6 Lens 3 −2.114020933 0.065 Plastic 1.546 54.73 3.062 7 −8.702572502 0.659 8 Lens 4 −1.443833892 0.044 Plastic 1.545 55.99 −62.637 9 1.046350279 0.441 10 IR-bands 0.864042638 0.509 BK7_SCHOTT 1.517 64.13 top filter 11 1E+18 0.460 12 1E+18 0.442 13 Image 1E+18 0.000 Plane Reference wavelength = 555 nm; shield position: NA. As for the parameters of the aspheric surfaces of the third embodiment, reference is made to Table 6.

TABLE 6 Aspheric Coefficients Surface # 2 3 4 5 6 7 k = −1.570268E+02 −1.113454E+00 −7.078319E−01 6.377985E−01 −3.557391E+02 −3.180425E−02 A₄ = 7.414091E−01 −2.013401E−01 2.647716E−01 1.860352E−01 7.943358E−02 1.023638E−01 A₆ = −5.689046E+00 −6.739243E−02 1.508646E−01 −3.391051E−02 −2.653148E−01 −4.250698E−01 A₈ = 2.671994E+01 −7.869830E−02 −6.568912E−01 −1.999412E−01 9.554808E−02 1.022894E+00 A₁₀ = −6.961711E+01 −5.905324E−01 −1.581403E+00 8.367402E−02 4.522941E−02 −1.500365E+00 A₁₂ = 1.009240E+01 4.560031E−01 5.034122E+00 5.210922E−02 4.874849E−02 1.147604E+00 A₁₄ = 3.518142E+02 2.616964E−01 −3.133242E+00 −3.592195E−02 −2.377029E−02 −3.236086E−01 A₁₆ = −5.510646E+02 −8.189977E−02 1.486668E−01 −3.098303E−03 −1.778609E−02 6.458426E−03 Surface # 8 9 k = −3.034997E+00 −1.241897E+00 A₄ = −4.215180E−02 −2.177327E−01 A₆ = −2.740446E−01 −7.498102E−02 A₈ = 2.567490E−01 1.429667E−01 A₁₀ = −2.580493E−01 −8.362090E−02 A₁₂ = 2.240296E−01 2.615752E−02 A₁₄ = −9.866776E−02 −4.389922E−03 A₁₆ = 1.609659E−02 3.067255E−04

The presentation of the aspheric surface formula in the third embodiment is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are identical to those in the first embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 5 and Table 6.

Third embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.605  0.498  0.572  0.470  1.535  0.533  ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.782  1.367  0.868  1.066  0.427  2.145  ETL EBL EIN EIR PIR STP 3.950  1.272  2.678  0.367  0.509  2.238  EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.678  0.801  0.721  0.8994  1.4142  0.959  ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.168  0.109  0.256  0.742  1.675  5.799  InRS41 InRS42 HVT41 HVT42 ODT % TDT % −0.00986   0.18415 0.88751 1.25373 2.25359 1.64974 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 1.40568 1.30249 0.77837 0.03806 0.92659 0.59760 ΣPPR ΣNPR ΣPPR/| ΣNPR | ΣPP ΣNP f1/ΣPP 2.08086 1.44374 1.44130 1.23231 −60.94075    −1.48510   f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f −0.02783   0.09490 0.02738 0.01851 0.27637 0.18511 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL 2.57367 3.98790 1.75833 0.98966 0.64537 0.86960 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 2.74506 0.73676 2.12408 1.49302 0.05997 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS 0.0223  0.4173  0.5528  0.3144  MTFQ0 MTFQ3 MTFQ7 MTFH0 MTFH3 MTFH7 0.75   0.67   0.22   0.52   0.37   0.13  

The following contents may be deduced from Table 5 and Table 6.

Values Related to Inflection Point of Third Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.3935 HIF111/HOI 0.1735 SGI111 0.0250 |SGI111|/(|SGI111| + TP1) 0.0313 HIF311 0.8726 HIF311/HOI 0.3847 SGI311 −0.0513 |SGI311|/(|SGI311| + TP3) 0.0722 HIF312 1.0150 HIF312/HOI 0.4475 SGI312 −0.0739 |SGI312|/(|SGI312| + TP3) 0.1009 HIF321 0.8958 HIF321/HOI 0.3950 SGI321 −0.3008 |SGI321|/(|SGI321| + TP3) 0.3135 HIF411 0.5144 HIF411/HOI 0.2268 SGI411 0.1068 |SGI411|/(|SGI411| + TP4) 0.1949 HIF421 0.6047 HIF421/HOI 0.2666 SGI421 0.1750 |SGI421|/(|SGI421| + TP4) 0.2839

The Fourth Embodiment (Embodiment 4)

Please refer to FIG. 4A, FIG. 4B, and FIG. 4C. FIG. 4A is a schematic view of the optical image capturing system according to the fourth embodiment of the present application, FIG. 4B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the fourth embodiment of the present application, and FIG. 4C is a characteristic diagram of modulation transfer of a visible light spectrum according to the fourth embodiment of the present application. As shown in FIG. 4A, in the order from an object side to an image side, the optical image capturing system includes an aperture stop 400, first lens element 410, a second lens element 420, a third lens element 430, a fourth lens element 440, an IR-bandstop filter 470, an image plane 480, and an image sensing device 490.

The first lens element 410 has positive refractive power and it is made of plastic material. The first lens element 410 has a convex object-side surface 412 and a convex image-side surface 414, and both of the object-side surface 412 and the image-side surface 414 are aspheric, and the object-side surface 412 has an inflection point.

The second lens element 420 has negative refractive power and it is made of plastic material. The second lens element 420 has a concave object-side surface 422 and a convex image-side surface 424, and both of the object-side surface 422 and the image-side surface 424 are aspheric.

The third lens element 430 has positive refractive power and it is made of plastic material. The third lens element 430 has a concave object-side surface 432 and a convex image-side surface 434, and both of the object-side surface 432 and the image-side surface 434 are aspheric, The object-side surface 432 has two inflection points, and the image-side surface 434 has an inflection point.

The fourth lens element 440 has positive refractive power and it is made of plastic material. The fourth lens element 440 has a convex object-side surface 442 and a concave image-side surface 444, and both of the object-side surface 442 and the image-side surface 444 are aspheric, and each of them has one inflection point.

The IR-bandstop filter 470 is made of glass material. The IR-bandstop filter 470 is disposed between the fourth lens element 440 and the image plane 480 without affecting the focal length of the optical image capturing system.

Please refer to the following Table 7 and Table 8.

The detailed data of the optical image capturing system of the fourth embodiment is as shown in Table 7.

TABLE 7 Lens Parameters for the Fourth Embodiment f = 1.85348 mm, f/HEP = 2.45, HAF = 45.7953 deg, Central Refractive Focal Surface# Curvature Radius Thickness Material Index Abbe # length 0 Object 1E+18 600 1 Ape. Stop/ 2.752142579 0.489 Plastic 1.544 56.09 1.775 Lens 1 2 −1.401261263 0.146 3 Lens 2 −1.243367523 0.260 Plastic 1.636 23.89 −4.549 4 −2.346492772 0.083 5 Lens 3 −0.727550985 0.499 Plastic 1.535 56.27 16.520 6 −0.833416754 0.057 7 Lens 4 0.649408322 0.349 Plastic 1.544 56.09 5.682 8 0.665603437 0.324 9 IR-bandstop 1E+18 0.350 BK7_SCHOTT 1.517 64.13 filter 10 1E+18 0.698 11 Image 1E+18 0.000 plane Reference wavelength = 555 nm; shield position: The 2^(nd) surface with clear aperture of 0.516 mm; the 3^(rd) surface with clear aperture of 0.549 mm. As for the parameters of the aspheric surfaces of the fourth embodiment, reference is made to Table 8.

TABLE 8 Aspheric Coefficients Surface # 1 2 3 4 5 6 k = −1.570268E+02 −1.113454E+00 −7.078319E−01 6.377985E−01 −3.557391E+02 −3.180425E−02 A₄ = 7.414091E−01 −2.013401E−01 2.647716E−01 1.860352E−01 7.943358E−02 1.023638E−01 A₆ = −5.689046E+00 −6.739243E−02 1.508646E−01 −3.391051E−02 −2.653148E−01 −4.250698E−01 A₈ = 2.671994E+01 −7.869830E−02 −6.568912E−01 −1.999412E−01 9.554808E−02 1.022894E+00 A₁₀ = −6.961711E+01 −5.905324E−01 −1.581403E+00 8.367402E−02 4.522941E−02 −1.500365E+00 A₁₂ = 1.009240E+01 4.560031E−01 5.034122E+00 5.210922E−02 4.874849E−02 1.147604E+00 A₁₄ = 3.518142E+02 2.616964E−01 −3.133242E+00 −3.592195E−02 −2.377029E−02 −3.236086E−01 A₁₆ = −5.510646E+02 −8.189977E−02 1.486668E−01 −3.098303E−03 −1.778609E−02 6.458426E−03 Surface # 7 8 k = −3.034997E+00 −1.241897E+00 A₄ = −4.215180E−02 −2.177327E−01 A₆ = −2.740446E−01 −7.498102E−02 A₈ = 2.567490E−01 1.429667E−01 A₁₀ = −2.580493E−01 −8.362090E−02 A₁₂ = 2.240296E−01 2.615752E−02 A₁₄ = −9.866776E−02 −4.389922E−03 A₁₆ = 1.609659E−02 3.067255E−04

The presentation of the aspheric surface formula in the fourth embodiment is similar to that in the first embodiment. Besides the definitions of parameters in following tables are identical to those in the first embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 7 and Table 8.

Fourth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.405  0.327  0.456  0.363  1.019  0.386  ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.827  1.259  0.914  1.042  0.635  1.551  ETL EBL EIN EIR PIR STP 3.221  1.285  1.936  0.247  0.324  1.597  EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.601  0.801  0.761  0.9369  1.3716  0.971  ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.109  0.107  0.169  0.749  1.295  2.976  InRS41 InRS42 HVT41 HVT42 ODT % TDT % 0.14470 0.18571 0.88312 1.06366 −0.93432   1.47772 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 1.04434 0.40749 0.11219 0.32621 0.39019 0.27533 ΣPPR ΣNPR ΣPPR/| ΣNPR | ΣPP ΣNP f1/ΣPP 0.51969 1.37056 0.37918 11.97179  7.45656 −0.37994   f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f 0.23802 0.07878 0.04470 0.03064 0.26938 0.18819 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL 1.88250 3.25408 1.67563 0.99444 0.57850 0.84827 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 2.44700 0.81236 1.88450 1.43137 0.09842 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS 0.4148  0.5324  0.5477  0.3269  MTFQ0 MTFQ3 MTFQ7 MTFH0 MTFH3 MTFH7 0.78   0.57   0.5   0.59   0.27   0.2   

The following contents may be deduced from Table 7 and Table 8.

Values Related to Inflection Point of Fourth Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.2708 HIF111/HOI 0.1395 SGI111 0.0117 |SGI111|/(|SGI111| + TP1) 0.0234 HIF311 0.2768 HIF311/HOI 0.1425 SGI311 −0.0349 |SGI311|/(|SGI311| + TP3) 0.0653 HIF312 0.7206 HIF312/HOI 0.3711 SGI312 −0.0980 |SGI312|/(|SGI312| + TP3) 0.1641 HIF321 0.6076 HIF321/HOI 0.3129 SGI321 −0.2188 |SGI321|/(|SGI321| + TP3) 0.3047 HIF411 0.4594 HIF411/HOI 0.2366 SGI411 0.1280 |SGI411|/(|SGI411| + TP4) 0.2685 HIF421 0.5033 HIF421/HOI 0.2592 SGI421 0.1505 |SGI421|/(|SGI421| + TP4) 0.3015

The Fifth Embodiment (Embodiment 5)

Please refer to FIG. 5A, FIG. 5B, and FIG. 5C. FIG. 5A is a schematic view of the optical image capturing system according to the fifths embodiment of the present application, FIG. 5B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the fifth embodiment of the present application, and FIG. 5C is a characteristic diagram of modulation transfer of a visible light spectrum according to the fifth embodiment of the present application. As shown in FIG. 5A, in the order from an object side to an image side, the optical image capturing system includes an aperture stop 500, a first lens element 510, a second lens element 520, a third lens element 530, a fourth lens element 540, an IR-bandstop filter 570, an image plane 580, and an image sensing device 590.

The first lens element 510 has positive refractive power and it is made of plastic material. The first lens element 510 has a convex object-side surface 512 and a convex image-side surface 514, and both of the object-side surface 512 and the image-side surface 514 are aspheric. The object-side surface 512 has one inflection point.

The second lens element 520 has negative refractive power and it is made of plastic material. The second lens element 520 has a concave object-side surface 522 and a convex image-side surface 524, and both of the object-side surface 522 and the image-side surface 524 are aspheric. The image-side surface 524 has two inflection points.

The third lens element 530 has positive refractive power and it is made of plastic material. The third lens element 530 has a concave object-side surface 532 and a convex image-side surface 534, and both of the object-side surface 532 and the image-side surface 534 are aspheric. The object-side surface 532 has three inflection points and the image-side surface 534 has an inflection point.

The fourth lens element 540 has negative refractive and it is made of plastic material. The fourth lens element 540 has a convex object-side surface 542 and a concave image-side surface 544, and both of the object-side surface 542 and the image-side surface 544 are aspheric, and each of them has one inflection point.

The IR-bandstop filter 570 is made of glass material. The IR-bandstop filter 570 is disposed between the fourth lens element 540 and the image plane 580 without affecting the focal length of the optical image capturing system.

Please refer to the following Table 9 and Table 10.

The detailed data of the optical image capturing system of the fifth embodiment is as shown in Table 9.

TABLE 9 Lens Parameters for the Fifth Embodiment f = 1.41712 mm, f/HEP = 2.0, HAF = 47.4999 deg Central Refractive Focal Surface# Curvature Radius Thickness Material Index Abbe # length 0 Object 1E+18 600 1 Ape. Stop 1E+18 −0.018 Plastic 1.545 55.96 2.656 2 Lens 1 1.837526577 0.299 3 −6.50045618 −0.149 4 1E+18 0.232 5 Lens 2 −6.980018034 0.255 Plastic 1.642 22.46 −12.881 6 −43.36046101 0.097 7 Lens 3 −1.019879926 0.469 Plastic 1.545 55.96 1.934 8 −0.603339037 0.030 9 Lens 4 0.660686054 0.255 Plastic 1.642 22.46 −11.422 10 0.514501534 0.358 11 IR-bandstop 1E+18 0.300 BK_7 1.517 64.13 filter 12 1E+18 0.345 13 1E+18 0.000 14 Image plane 1E+18 0.000 Reference wavelength = 555 nm; shield position: The 4^(th) surface with clear aperture of 0.450 mm. As for the parameters of the aspheric surfaces of the fifth embodiment, reference is made to Table 10.

TABLE 10 Aspheric Coefficients Surface # 2 3 5 6 7 8 k = −9.000000E+01 9.483066E−01 3.225514E−01 1.441165E+01 −3.677517E+01 −9.744549E−01 A₄ = 3.101628E+00 −1.161072E+00 −1.525013E+00 1.853977E+00 −4.483200E−01 1.407761E+00 A₆ = −8.703098E+01 −8.060658E+00 −1.642943E+01 −2.285534E+01 2.471678E+01 −1.468684E+01 A₈ = 2.085506E+03 −1.811218E−01 2.415323E+02 1.876663E+02 −1.970610E+02 1.323308E+02 A₁₀ = −3.681218E+04 3.793590E+02 −4.468484E+03 −1.376081E+03 7.010136E+02 −7.644766E+02 A₁₂ = 4.401183E+05 −2.751815E+03 4.808522E+04 7.155486E+03 −8.377075E+02 2.787540E+03 A₁₄ = −3.449010E+06 7.558383E+03 −2.928948E+05 −2.403871E+04 −2.097381E+03 −6.283881E+03 A₁₆ = 1.685941E+07 −7.443102E+03 1.022023E+06 4.863839E+04 8.620885E+03 8.497906E+03 A₁₈ = −4.653513E+07 0.000000E+00 −1.908429E+06 −5.363574E+04 −1.138371E+04 −6.344258E+03 A₂₀ = 5.530850E+07 0.000000E+00 1.474465E+06 2.475150E+04 5.614807E+03 2.024783E+03 Surface # 8 9 k = −1.631753E+00 −3.294076E+00 A₄ = −8.869628E−02 7.248669E−01 A₆ = −4.276729E−01 −2.385662E+00 A₈ = −2.388386E+00 3.713935E−01 A₁₀ = 1.077529E+01 7.863415E+00 A₁₂ = −3.277948E+01 −1.608676E+01 A₁₄ = 7.123470E+01 1.579069E+01 A₁₆ = −9.180513E+01 −8.683362E+00 A₁₈ = 6.176906E+01 2.579379E+00 A₂₀ = −1.675653E+01 −3.248012E−01

The presentation of the aspheric surface formula in the fifth embodiment is similar to that in the first embodiment. Besides the definitions of parameters in following tables are identical to those in the first embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 9 and Table 10.

Fifth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.228  0.311  0.402  0.273  1.093  0.350  ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.764  1.221  0.856  1.072  0.307  1.215  ETL EBL EIN EIR PIR STP 2.460  0.896  1.564  0.251  0.358  1.278  EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.636  0.776  0.701  0.8931  1.0033  0.950  ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.071  0.065  0.213  0.863  0.675  7.091  InRS41 InRS42 HVT41 HVT42 ODT % TDT % 0.16194 0.26500 0.75534 0.92083 2.00085 2.66025 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 0.53354 0.11002 0.73262 0.12407 0.20620 6.65920 ΣPPR ΣNPR ΣPPR/| ΣNPR | ΣPP ΣNP f1/ΣPP 0.84263 0.65761 1.28135 −10.94677    −8.76615   1.17670 f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f −0.30299   0.05842 0.06830 0.02117 0.33114 0.17994 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL 1.48756 2.49088 1.61536 0.99281 0.59720 0.85911 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 1.49605 0.60733 1.17138 1.84027 0.11789 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS 0.6350  1.0392  0.5972  0.3697  MTFQ0 MTFQ3 MTFQ7 MTFH0 MTFH3 MTFH7 0.74   0.58   0.37   0.5247  0.3   0.08  

The following contents may be deduced from Table 9 and Table 10.

Values Related to Inflection Point of Fifth Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.2894 HIF111/HOI 0.1877 SGI111 0.0224 |SGI111|/(|SGI111| + TP1) 0.0698 HIF221 0.0327 HIF221/HOI 0.0212 SGI221 −0.0000 |SGI221|/(|SGI221| + TP2) 0.0000 HIF222 0.2586 HIF222/HOI 0.1677 SGI222 0.0031 |SGI222|/(|SGI222| + TP2) 0.0121 HIF311 0.1829 HIF311/HOI 0.1186 SGI311 −0.0131 |SGI311|/(|SGI311| + TP3) 0.0271 HIF312 0.4513 HIF312/HOI 0.2927 SGI312 −0.0263 |SGI312|/(|SGI312| + TP3) 0.0530 HIF313 0.6540 HIF313/HOI 0.4241 SGI313 −0.0614 |SGI313|/(|SGI313| + TP3) 0.1157 HIF321 0.5054 HIF321/HOI 0.3277 SGI321 −0.1780 |SGI321|/(|SGI321| + TP3) 0.2750 HIF411 0.4469 HIF411/HOI 0.2898 SGI411 0.1329 |SGI411|/(|SGI411| + TP4) 0.3426 HIF421 0.4576 HIF421/HOI 0.2967 SGI421 0.1646 |SGI421|/(|SGI421| + TP4) 0.3923

The Sixth Embodiment (Embodiment 6)

Please refer to FIG. 6A, FIG. 6B, and FIG. 6C. FIG. 6A is a schematic view of the optical image capturing system according to the sixth Embodiment of the present application, FIG. 6B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the sixth Embodiment of the present application, and FIG. 6C is a characteristic diagram of modulation transfer of a visible light spectrum according to the sixth embodiment of the present application. As shown in FIG. 6A, in the order from an object side to an image side, the optical image capturing system includes an aperture stop 600, a first lens element 610, a second lens element 620, a third lens element 630, a fourth lens element 640, an IR-bandstop filter 670, an image plane 680, and an image sensing device 690.

The first lens element 610 has positive refractive power and it is made of plastic material. The first lens element 610 has a convex object-side surface 612 and a convex image-side surface 614, and both of the object-side surface 612 and the image-side surface 614 are aspheric. The object-side surface 612 has an inflection point.

The second lens element 620 has negative refractive power and it is made of plastic material. The second lens element 620 has a concave object-side surface 622 and a convex image-side surface 624, and both of the object-side surface 622 and the image-side surface 624 are aspheric. The object-side surface 622 has two inflection points and the image-side surface 624 has an inflection point.

The third lens element 630 has positive refractive power and it is made of plastic material. The third lens element 630 has a concave object-side surface 632 and a convex image-side surface 634, and both of the object-side surface 632 and the image-side surface 634 are aspheric. The object-side surface 632 has two inflection points and the image-side surface 634 has three inflection points.

The fourth lens element 640 has positive refractive power and it is made of plastic material. The fourth lens element 640 has a convex object-side surface 642 and a concave image-side surface 644, and both of the object-side surface 642 and the image-side surface 644 are aspheric, and each of them has an inflection point.

The IR-bandstop filter 670 is made of glass material. The IR-bandstop filter 670 is disposed between the fourth lens element 640 and the image plane 680 without affecting the focal length of the optical image capturing system.

Please refer to the following Table 11 and Table 12.

The detailed data of the optical image capturing system of the sixth Embodiment is as shown in Table 11.

TABLE 11 Lens Parameters for the Sixth Embodiment f = 1.04309 mm; f/HEP = 2.0; HAF = 44.0001 deg Central Refractive Focal Surface # Curvature Radius Thickness Material Index Abbe # length 0 Object 1E+18 600 1 Ape. Stop 1E+18 −0.012 2 Lens 1 1.000446988 0.186 Plastic 1.545 55.96 1.586 3 −6.0357696 −0.100 4 1E+18 0.176 5 Lens 2 −4.337545744 0.170 Plastic 1.642 22.46 −6.699 6 −28916.23724 0.079 7 Lens 3 −0.651972381 0.266 Plastic 1.545 55.96 2.388 8 −0.497406556 0.020 9 Lens 4 0.362732663 0.177 Plastic 1.642 22.46 15.065 10 0.304676592 0.216 11 IR-bandstop 1E+18 0.200 BK_7 1.517 64.13 1E+18 filter 12 1E+18 0.260 13 1E+18 0.000 14 Image 1E+18 0.000 plane Reference wavelength = 555 nm; shield position: The 4^(th) surface with clear aperture of 0.300 mm. As for the parameters of the aspheric surfaces of the sixth Embodiment, reference is made to Table 12.

TABLE 12 Aspheric Coefficients Surface # 2 3 5 6 7 8 k = −9.000000E+01 9.483066E−01 3.225514E−01 1.441165E+01 −4.447187E+01 −1.001136E+00 A₄ = 1.310232E+01 −4.764985E+00 −4.212068E+00 5.826507E+00 −5.513197E−01 2.309595E+00 A₆ = −7.444401E+02 2.219860E+01 −8.986938E+01 −1.770184E+02 1.756014E+02 −6.824750E+01 A₈ = 3.707345E+04 −1.586250E+03 3.949905E+03 3.421422E+03 −3.162749E+03 2.141488E+03 A₁₀ = −1.429154E+06 3.034595E+04 −1.685039E+05 −5.616148E+04 2.463516E+04 −3.013814E+04 A₁₂ = 3.812720E+07 −2.946738E+05 4.146685E+06 6.427338E+05 −6.044917E+04 2.452718E+05 A₁₄ = −6.712446E+08 1.471009E+06 −5.700304E+07 −4.735831E+06 −4.318123E+05 −1.228633E+06 A₁₆ = 7.382635E+09 −3.259289E+06 4.475375E+08 2.129845E+07 3.775033E+06 3.721181E+06 A₁₈ = −4.584926E+10 0.000000E+00 −1.880301E+09 −5.284522E+07 −1.121592E+07 −6.250752E+06 A₂₀ = 1.226100E+11 0.000000E+00 3.268649E+09 5.487006E+07 1.244712E+07 4.488617E+06 Surface # 9 10 k = −2.632225E+00 −3.271975E+00 A₄ = −3.720217E+00 −3.619313E−01 A₆ = 4.865481E+01 3.087579E+00 A₈ = −4.534249E+02 −7.001472E+01 A₁₀ = 2.505701E+03 4.578605E+02 A₁₂ = −9.184997E+03 −1.577881E+03 A₁₄ = 2.420553E+04 3.198959E+03 A₁₆ = −4.714450E+04 −3.841218E+03 A₁₈ = 6.085866E+04 2.541362E+03 A₂₀ = −3.714651E+04 −7.200315E+02

In the sixth Embodiment, the presentation of the aspheric surface formula is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are identical to those in the first embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 11 and Table 12.

Sixth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.129  0.209  0.220  0.189  1.133  0.284  ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.694  1.230  0.828  1.070  0.416  0.748  ETL EBL EIN EIR PIR STP 1.624  0.592  1.032  0.132  0.216  0.799  EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.635  0.724  0.614  0.8764  0.6755  0.936  ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 11.613   0.420  0.051  0.984  8.398  0.655  InRS41 InRS42 HVT41 HVT42 ODT % TDT % 0.10161 0.14320 0.50311 0.59538 1.54930 1.38394 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 0.65775 0.15572 0.43677 0.06924 0.23674 2.80487 ΣPPR ΣNPR ΣPPR/| ΣNPR | ΣPP ΣNP f1/ΣPP 0.22496 1.09452 0.20553 8.36674 3.97403 1.80062 f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f 0.39905 0.07299 0.07599 0.01917 0.25511 0.16923 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL 0.97447 1.64999 1.60505 0.99276 0.59059 0.82001 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 1.54464 0.73850 1.09679 1.50752 0.15380 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS 0.5756  0.8113  0.5792  0.3608  MTFQ0 MTFQ3 MTFQ7 MTFH0 MTFH3 MTFH7 0.79   0.73   0.62   0.58   0.49   0.34  

The following contents may be deduced from Table 11 and Table 12.

Values Related to Inflection Point of Sixth Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.1916 HIF111/HOI 0.1863 SGI111 0.0172 |SGI111|/(|SGI111| + TP1) 0.0844 HIF211 0.2995 HIF211/HOI 0.2913 SGI211 −0.0563 |SGI211|/(|SGI211| + TP2) 0.2487 HIF212 0.3239 HIF212/HOI 0.3151 SGI212 −0.0693 |SGI212|/(|SGI212| + TP2) 0.2896 HIF221 0.1674 HIF221/HOI 0.1629 SGI221 0.0021 |SGI221|/(|SGI221| + TP2) 0.0121 HIF311 0.1118 HIF311/HOI 0.1088 SGI311 −0.0075 |SGI311|/(|SGI311| + TP3) 0.0272 HIF312 0.2967 HIF312/HOI 0.2887 SGI312 −0.0120 |SGI312|/(|SGI312| + TP3) 0.0433 HIF321 0.2464 HIF321/HOI 0.2397 SGI321 −0.0544 |SGI321|/(|SGI321| + TP3) 0.1697 HIF322 0.3984 HIF322/HOI 0.3876 SGI322 −0.1027 |SGI322|/(|SGI322| + TP3) 0.2784 HIF323 0.4701 HIF323/HOI 0.4573 SGI323 −0.1233 |SGI323|/(|SGI323| + TP3) 0.3167 HIF411 0.2801 HIF411/HOI 0.2725 SGI411 0.0791 |SGI411|/(|SGI411| + TP4) 0.3094 HIF421 0.2848 HIF421/HOI 0.2770 SGI421 0.0950 |SGI421|/(|SGI421| + TP4) 0.3500

The above-mentioned descriptions represent merely the exemplary embodiment of the present disclosure, without any intention to limit the scope of the present disclosure thereto. Various equivalent changes, alternations or modifications based on the claims of present disclosure are all consequently viewed as being embraced by the scope of the present disclosure. 

What is claimed is:
 1. An optical image capturing system, from an object side to an image side, comprising: a first lens element with refractive power, both of the object-side surface and the image-side surface of the first lens element are convex surface on the optical axis; a second lens element with refractive power; a third lens element with refractive power; a fourth lens element with refractive power; and an image plane, the optical image capturing system comprises four lens elements with refractive powers; at least one lens element among the first to the fourth lens elements has positive refractive power; focal lengths of the first through the fourth lens elements are respectively f1, f2, f3 and f4; a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, and a distance on the optical axis from the object-side surface of the first lens element to the image plane is HOS; a distance on the optical axis from the object-side surface of the first lens element to an image-side surface of the fourth lens element is InTL; half of a maximum angle of view of the optical image capturing system is HAF; thicknesses paralleling the optical axis, of the first lens element, of the second lens element, of the third lens element and of the fourth lens element at height of ½ HEP respectively are ETP1, ETP2, ETP3 and ETP4; a sum of the ETP1 to the ETP4 is SETP, thicknesses of the first lens element, the second lens element, the third lens element and the fourth lens element on the optical axis respectively are TP1, TP2, TP3 and TP4; a sum of the TP1 to the TP4 is STP, and the following conditions are satisfied: 1.0≦f/HEP≦10; 0 deg<HAF≦150 deg and 0.5≦SETP/STP<1.
 2. The optical image capturing system of claim 1, wherein a horizontal distance in parallel with the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the image plane is ETL. A horizontal distance in parallel with the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN. The following condition is satisfied: 0.2≦EIN/ETL<1.
 3. The optical image capturing system of claim 1, wherein a horizontal distance in parallel with the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN, and the following condition is satisfied: 0.3≦SETP/EIN<1.
 4. The optical image capturing system of claim 1, wherein the optical image capturing system comprises a light filtering element, and the light filtering element is located between the fourth lens element and the image plane; a distance in parallel with the optical axis, from a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP to the light filtering element, is EIR; a distance in parallel with the optical axis, from an axial point on the image-side surface of the fourth lens element to the light filtering element, is PIR, and the following condition is satisfied: 0.1≦EIR/PIR<1.1.
 5. The optical image capturing system of claim 1, wherein the optical image capturing system has a maximum image height HOI on the image plane perpendicular to the optical axis, the following condition is satisfied: 1.5≦HOS/HOI≧1.9.
 6. The optical image capturing system of claim 1, wherein the first lens element has positive refractive power and the second lens element has negative refractive power.
 7. The optical image capturing system of claim 1, wherein the optical image capturing system has a maximum image height HOI on the image plane perpendicular to the optical axis, contrast transfer rates of modulation transfer of visible light at spatial frequency of 110 cycles/mm at positions of the optical axis, 0.3 HOI and 0.7 HOI on the image plane are respectively denoted by MTFQ0, MTFQ3 and MTFQ7, and conditions as follows are satisfied: MTFQ0≧0.2, MTFQ3≧0.01, and MTFQ7≧0.01.
 8. The optical image capturing system of claim 1, wherein a horizontal distance in parallel with the optical axis from a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP to the image plane is EBL, a horizontal distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the image plane is BL, and the following condition is satisfied: 0.1≦EBL/BL<1.5.
 9. The optical image capturing system of claim 1, further comprising an aperture stop, a distance from the aperture stop to the image plane on the optical axis is InS, and the following condition is satisfied: 0.2≦InS/HOS≦1.1.
 10. An optical image capturing system, from an object side to an image side, comprising: a first lens element with refractive power, an object-side surface and an image-side surface of the first lens element on the optical axis are both convex surface; a second lens element with refractive power, an image-side surface of the second lens element on the optical axis is convex surface; a third lens element with refractive power, an image-side surface of the third lens element on the optical axis is convex surface; a fourth lens element with refractive power; and an image plane; the optical image capturing system comprises four lens elements with refractive powers; at least one lens element among the second to the fourth lens elements has positive refractive power; focal lengths of the first through the fourth lens elements are respectively f1, f2, f3 and f4; a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, and a distance on the optical axis from the object-side surface of the first lens element to the image plane is HOS; a distance on the optical axis from the object-side surface of the first lens element to an image-side surface of the fourth lens element is InTL; half of a maximum angle of view of the optical image capturing system is HAF; a horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the image plane is ETL; a horizontal distance paralleling the optical axis from the coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN; and condition as follows is satisfied: 1.0≦f/HEP≦10, 0 deg<HAF≦150 deg and 0.2≦EIN/ETL<1.
 11. The optical image capturing system of claim 10, wherein a horizontal distance in parallel with the optical axis from a coordinate point on an image-side surface of the first lens element at height of ½ HEP to a coordinate point on an object-side surface of the second lens element at height of ½ HEP is ED12, a distance from the first lens element to the second lens element on the optical axis is IN12, and the following condition is satisfied: 0<ED12/IN12≦35.
 12. The optical image capturing system of claim 10, wherein the first lens element has positive refractive power and the second lens element has negative refractive power.
 13. The optical image capturing system of claim 10, wherein the central thicknesses of the second lens element and the third lens element on the optical axis are TP2 and TP3, respectively, the following condition is satisfied: 0.4≦TP2/TP3≦3.
 14. The optical image capturing system of claim 10, wherein an object-side surface of the third lens element has at least two inflection points.
 15. The optical image capturing system of claim 10, wherein a distance on the optical axis between the first lens element and the second lens element is denoted as IN12, and a distance on the optical axis between the second lens element and the third lens element is denoted as IN23, and the following condition is satisfied: 0<IN12/IN23≦5.
 16. The optical image capturing system of claim 10, wherein the central thicknesses of the first lens element and the third lens element on the optical axis are TP1 and TP3, respectively, the following condition is satisfied: 0.5≦TP1/TP3≦1.5.
 17. The optical image capturing system of claim 10, wherein the central thicknesses of the forth lens element and the third lens element on the optical axis are TP4 and TP3, respectively, the following condition is satisfied: 0.5≦TP4/TP3≦5.
 18. The optical image capturing system of claim 10, wherein the optical image capturing system has a maximum image height HOI on the image plane perpendicular to the optical axis, contrast transfer rates of modulation transfer of visible light at spatial frequency of 220 cycles/mm at positions of the optical axis, 0.3 HOI and 0.7 HOI on the image plane are respectively denoted by MTFH0, MTFH3 and MTFH7, and conditions as follows are satisfied: MTFH0≧0.2, MTFH3≧0.01, and MTFH7≧0.01.
 19. The optical image capturing system of claim 10, wherein at least one lens element among the first lens element, the second lens element, the third lens element and the fourth lens elements is a filter element of light with a wavelength of less than 500 nm.
 20. An optical image capturing system, from an object side to an image side, comprising: a first lens element with refractive power, an object-side surface and an image-side surface of the first lens element on the optical axis are both convex surface; a second lens element with refractive power, an image-side surface of the second lens element on the optical axis is convex surface; a third lens element with refractive power, an image-side surface of the third lens element on the optical axis is convex surface, and an object-side of the third lens element has at least two inflection points; a fourth lens element with refractive power; and an image plane, the optical image capturing system comprises four lens elements with refractive powers; focal lengths of the first through the fourth lens elements are respectively f1, f2, f3 and f4; a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, and a distance on the optical axis from the object-side surface of the first lens element to the image plane is HOS; a distance on the optical axis from the object-side surface of the first lens element to an image-side surface of the fourth lens element is InTL; half of a maximum angle of view of the optical image capturing system is HAF; a horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the image plane is ETL; a horizontal distance paralleling the optical axis from the coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN; and condition as follows is satisfied: 1.0≦f/HEP≦10.0, 0 deg<HAF≦100 deg and 0.2≦EIN/ETL<1.
 21. The optical image capturing system of claim 20, wherein the first lens element has positive refractive power; the second lens element has negative refractive power and the third lens element has positive refractive power.
 22. The optical image capturing system of claim 20, wherein the central thicknesses of the first lens element and the third lens element on the optical axis are TP1 and TP3, respectively, the following condition is satisfied: 1.3≦TP1/TP3≦1.5.
 23. The optical image capturing system of claim 20, wherein the central thicknesses of the second lens element and the third lens element on the optical axis are TP2 and TP3, respectively, the following condition is satisfied: 0.6≦TP2/TP3≦0.9.
 24. The optical image capturing system of claim 20, wherein the central thicknesses of the forth lens element and the third lens element on the optical axis are TP4 and TP3, respectively, the following condition is satisfied: 0.6≦T4/TP3≦0.9.
 25. The optical image capturing system of claim 20, further comprising an aperture stop, an image sensing device and a driving module, wherein the image sensing device is disposed on the image plane, a distance on the optical axis from the aperture stop to the image plane is InS, and the driving module couples with the lens elements to displace the lens elements; the following condition is satisfied: 0.2≦InS/HOS≦1.1. 